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root/group/trunk/langevinHull/langevinHull.bib
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fixed a few references

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# Content
1 %% This BibTeX bibliography file was created using BibDesk.
2 %% http://bibdesk.sourceforge.net/
3
4
5 %% Created for Dan Gezelter at 2010-10-18 12:52:34 -0400
6
7
8 %% Saved with string encoding Unicode (UTF-8)
9
10
11 @string{acp = {Adv. Chem. Phys.}}
12
13 @string{bj = {Biophys. J.}}
14
15 @string{ccp5 = {CCP5 Information Quarterly}}
16
17 @string{cp = {Chem. Phys.}}
18
19 @string{cpl = {Chem. Phys. Lett.}}
20
21 @string{jacs = {J. Am. Chem. Soc.}}
22
23 @string{jcc = {J. Comp. Chem.}}
24
25 @string{jcop = {J. Comp. Phys.}}
26
27 @string{jcp = {J. Chem. Phys.}}
28
29 @string{jmb = {J. Mol. Bio.}}
30
31 @string{jml = {J. Mol. Liq.}}
32
33 @string{jpc = {J. Phys. Chem.}}
34
35 @string{jpca = {J. Phys. Chem. A}}
36
37 @string{jpcb = {J. Phys. Chem. B}}
38
39 @string{mp = {Mol. Phys.}}
40
41 @string{pams = {Proc. Am. Math Soc.}}
42
43 @string{pccp = {Phys. Chem. Chem. Phys.}}
44
45 @string{pnas = {Proc. Natl. Acad. Sci. USA}}
46
47 @string{pr = {Phys. Rev.}}
48
49 @string{pra = {Phys. Rev. A}}
50
51 @string{prb = {Phys. Rev. B}}
52
53 @string{pre = {Phys. Rev. E}}
54
55 @string{prl = {Phys. Rev. Lett.}}
56
57 @string{rmp = {Rev. Mod. Phys.}}
58
59
60 @misc{openmd,
61 Author = {J. Daniel Gezelter and Shenyu Kuang and James Marr and Kelsey Stocker and Chunlei Li and Charles F. Vardeman and Teng Lin and Christopher J. Fennell and Xiuquan Sun and Kyle Daily and Yang Zheng and Matthew A. Meineke},
62 Date-Added = {2010-10-18 12:51:55 -0400},
63 Date-Modified = {2010-10-18 12:51:55 -0400},
64 Howpublished = {Available at {\tt http://openmd.net}},
65 Title = {{OpenMD, an open source engine for molecular dynamics}}}
66
67 @article{Fine1973,
68 Author = {Fine, Rana A. and Millero, Frank J.},
69 Date-Added = {2010-09-22 15:53:25 -0400},
70 Date-Modified = {2010-09-22 15:53:25 -0400},
71 Journal = {J. Chem. Phys.},
72 Keywords = {water; isothermal compressibility; experiment},
73 Number = {10},
74 Pages = {5529-5536},
75 Title = {Compressibility of water as a function of temperature and pressure},
76 Volume = {59},
77 Year = {1973},
78 Bdsk-File-1 = {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}}
79
80 @article{Pi2009,
81 Author = {Pi, Helena L. and Aragones, Juan L. and Vega, Carlos and Noya, Eva G. and Abascal, Jose L.F. and Gonzalez, Miguel A. and McBride,, Carl},
82 Date-Added = {2010-09-22 15:53:20 -0400},
83 Date-Modified = {2010-09-22 15:53:20 -0400},
84 Journal = {Mol. Phys.},
85 Keywords = {water; isothermal compressibility; density},
86 Number = {4},
87 Pages = {365-374},
88 Title = {Anomalies in water as obtained from computer simulations of the TIP4P/2005 model: Density maxima, and density, isothermal compressibility and heat capacity minima},
89 Volume = {107},
90 Year = {2009},
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92
93 @article{Grote1995,
94 Author = {Grote, Marcus J. and Keller, Joseph B.},
95 Date-Added = {2010-09-08 16:48:01 -0400},
96 Date-Modified = {2010-09-08 16:48:01 -0400},
97 Keywords = {boundary},
98 Title = {On nonreflecting boundary conditions},
99 Year = {1995},
100 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAZQAAAAAAZQAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+Q1Hcm90ZTE5OTUucGRmAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAElnryGojMAAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyGpbcAAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIAP1NlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6R3JvdGUxOTk1LnBkZgAADgAcAA0ARwByAG8AdABlADEAOQA5ADUALgBwAGQAZgAPABIACABTAGUAcgBlAG4AaQB0AHkAEgA2VXNlcnMva3N0b2NrZTEvRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9Hcm90ZTE5OTUucGRmABMAAS8AABUAAgAP//8AAIAF0hwdHh9YJGNsYXNzZXNaJGNsYXNzbmFtZaMfICFdTlNNdXRhYmxlRGF0YVZOU0RhdGFYTlNPYmplY3RfECouLi9Eb2N1bWVudHMvUmVzZWFyY2gvUGFwZXJzL0dyb3RlMTk5NS5wZGbSHB0kJaIlIVxOU0RpY3Rpb25hcnkSAAGGoF8QD05TS2V5ZWRBcmNoaXZlcgAIABEAFgAfACgAMgA1ADoAPABFAEsAUgBdAGUAbABvAHEAcwB2AHgAegB8AIYAkwCYAKACOAI6Aj8CSAJTAlcCZQJsAnUCogKnAqoCtwK8AAAAAAAAAgEAAAAAAAAAKAAAAAAAAAAAAAAAAAAAAs4=}}
101
102 @article{Warshel1978,
103 Author = {A. Warshel},
104 Date-Added = {2010-09-08 16:48:01 -0400},
105 Date-Modified = {2010-09-08 16:48:01 -0400},
106 Journal = {Chem. Phys. Lett.},
107 Keywords = {boundary; SCSSD},
108 Month = {May},
109 Number = {3},
110 Pages = {454-458},
111 Title = {A microscopic model for calculations of chemical processes in aqueous solutions},
112 Volume = {55},
113 Year = {1978},
114 Bdsk-File-1 = {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}}
115
116 @article{Belch1985,
117 Abstract = {The structure in a water cluster restrictedby a hydrophobic wall was studied as a function of the distance from the wall. Significant orientational preference was observed near the surface. This preference is very similar to that present in liquid water near planar hydrophobic surfaces of infinite extend.},
118 Author = {Belch, A.C. and Berkowitz, M.},
119 Date-Added = {2010-09-08 16:48:01 -0400},
120 Date-Modified = {2010-09-08 16:48:01 -0400},
121 Journal = {Chem. Phys. Lett.},
122 Keywords = {dewetting; boundary},
123 Month = {January},
124 Number = {3},
125 Pages = {278-282},
126 Title = {Molecular dynamics simulations of TIPS2 water restricted by a spherical hydrophobic boundary},
127 Volume = {113},
128 Year = {1985},
129 Bdsk-File-1 = {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}}
130
131 @article{King1989,
132 Abstract = {A consistent simulation of ionic or strongly polar solutes in polar solvents presents a major challenge from both fundamental and practical aspects. The frequently used method of periodic boundary conditions (PBC) does not correctly take into account the symmetry of the solute field. Instead of using PBC, it is natural to model this type of system as a sphere (with the solute at the origin), but the boundary conditions to be used in such a model are not obvious. Early calculations performed with our surface constrained soft sphere dipoles (SCSSD) model indicated that the dipoles near the surface ofthe sphere will show unusual orientational preferences (they will overpolarize) unless a corrective force is included in the model, and thus we implemented polarization constraints in this spherical model of polar solutions. More recent approaches that treated the surface with stochastic dynamics, but did not take into account the surface polarization effects, were also found to exhibit these nonphysical orientational preferences. The present work develops a surface constrained all- atom solvent (SCAAS) model in order to consistently treat the surface polarization effects in all-atom molecular dynamics simulations. The SCAAS model, which was presented in a preliminary way in previous works, introduces surface constraints as boundary conditions in order to make the necessarily finite system behave as if it was part of an infinite system. The performance of the model with regard to various properties of bulk water is examined by comparing its results to those obtained by PBC simulations. The results obtained from SCAAS models of different sizes are found to be similar to each other and to the corresponding PBC results. The performance of the model in simulations of solvated ions is emphasized and a comparison of the results obtained with spheres of different sizes demonstrates that the model does not possess significant size dependence. This indicates that the model can be used with a relatively small number of solvent molecules for convergent simulation of structure, energetics, and dynamics of polar solutions. The much simpler fixed center Langevin dipoles (FCLD) model is also examined and found to provide a powerful tool for estimating solvation free energies. Finally, a preliminary study of the dielectric properties of the SCAAS model is reported and the potential of this model for exploring the correct implementation of the solvent reaction field is discussed.},
133 Author = {King, G. and Warshel, A.},
134 Date-Added = {2010-09-08 16:48:01 -0400},
135 Date-Modified = {2010-09-08 16:48:01 -0400},
136 Journal = {J. Chem. Phys.},
137 Keywords = {dewetting; boundary},
138 Month = {September},
139 Number = {6},
140 Pages = {3647-3661},
141 Title = {A surface constrained all-atom solvent model for effective simulations of polar solutions},
142 Volume = {91},
143 Year = {1989},
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145
146 @article{Lee1984,
147 Abstract = {Molecular dynamics simulations have been carried out for liquid water between flat hydrophobic s~rf~ces. The surfaces p.rodu~edensity oscillations that extend at lea~t 10 A into the liquid, and slgmficant molecular onentatlOnal preferences that extend at least 7 A into the liquid. The liquid structure nearest the surface is characterized by "dangling" hydrogen bonds; i.e., a typical water molecule at the surface has one potentially hydrogen-bonding group oriented toward the hydrophobic surface. This surface arrangement represents a balance between the tendencies of the liquid to maximize the number of hydrogen bonds on the one hand, and to maximize the packing density of the molecules on the other. A detailed analysis shows that the structural properties of the liquid farther from the surface can be understood as effects imposed by this surface structure. These results show that the hydration structure of large hydrophobic surfaces
148 can be very different from that of small hydrophobic molecules.},
149 Author = {Lee, C.Y. and McCammon, J.A. and Rossky, P.J.},
150 Date-Added = {2010-09-08 16:48:01 -0400},
151 Date-Modified = {2010-09-08 16:48:01 -0400},
152 Journal = {J. Chem. Phys.},
153 Keywords = {dewetting; boundary},
154 Month = {May},
155 Number = {9},
156 Pages = {4448-4455},
157 Title = {The structure of liquid water at an extended hydrophobic surface},
158 Volume = {80},
159 Year = {1984},
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161
162 @article{Beglov1994,
163 Abstract = {An approach is developed to obtain statistical properties similar to those of an infinite bulk system from computer simulations of a finite cluster. A rigorous theoretical formulation is given for the solvent boundary potential which takes the influence of the surrounding bulk into account. The solvent boundary potential is the configuration-dependent solvation free energy of an effective cluster composed of an arbitrary solute and a finite number of explicit solvent molecules embedded inside a hard sphere of variable radius; the hard sphere does not act directly on the solute or the explicit solvent molecules, and its radius varies according to the instantaneous configurations. The formulation follows from an exact separation of the multidimensional configurational Boltzmann integral in terms of the solvent molecules nearest to the solute and the remaining bulk solvent molecules. An approximation to the solvent boundary potential is constructed for simulations of bulk water at constant pressure, including the influence of van der Waals and electrostatic interactions. The approximation is illustrated with calculations of the solvation free energy of a water molecule and of sodium and potassium ions. The influence of bulk solvent on the conformational equilibrium of molecular solutes is illustrated by performing umbrella sampling calculations of n-butane and alanine dipeptide in water. The boundary potential is tested to examine the dependence of the results on the number of water molecules included explicitly in the simulations. It is observed that bulk-like results are obtained, even when only the waters in the first hydration shell are included explicitly.},
164 Author = {Beglov, D. and Roux, B.},
165 Date-Added = {2010-09-08 16:48:01 -0400},
166 Date-Modified = {2010-09-08 16:48:01 -0400},
167 Journal = {J. Chem. Phys.},
168 Keywords = {dewetting; boundary},
169 Month = {June},
170 Number = {12},
171 Pages = {9050-9063},
172 Title = {Finite representations of an infinite bulk system: Solvent boundary potential for computer simulations},
173 Volume = {100},
174 Year = {1994},
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176
177 @article{Choudhury2007,
178 Author = {Niharendu Choudhury and B. Montgomery Pettitt},
179 Date-Added = {2010-09-08 16:48:01 -0400},
180 Date-Modified = {2010-09-08 16:48:01 -0400},
181 Journal = {J. Am. Chem. Soc.},
182 Keywords = {dewetting; hydrophobic},
183 Number = {15},
184 Pages = {4847-4852},
185 Title = {The dewetting transition and the hydrophobic effect},
186 Volume = {129},
187 Year = {2007},
188 Bdsk-File-1 = {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}}
189
190 @article{Du1994,
191 Author = {Quan Du and Eric Freysz and Y. Ron Shen},
192 Date-Added = {2010-09-08 16:48:01 -0400},
193 Date-Modified = {2010-09-08 16:48:01 -0400},
194 Journal = {Science},
195 Keywords = {dewetting; hydrophobic boundary},
196 Month = {May},
197 Pages = {826-828},
198 Title = {Surface vibrational spectroscopic studies of hydrogen bonding and hydrophobicity},
199 Volume = {264},
200 Year = {1994},
201 Bdsk-File-1 = {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}}
202
203 @article{Lee1994,
204 Author = {Song Hi Lee and Peter J. Rossky},
205 Date-Added = {2010-09-08 16:48:01 -0400},
206 Date-Modified = {2010-09-08 16:48:01 -0400},
207 Journal = {J. Chem. Phys.},
208 Keywords = {dewetting; hydrophobic boundary; hydrophilic boundary},
209 Month = {February},
210 Number = {4},
211 Pages = {3334-3345},
212 Title = {A comparison of the structure and dynamics of liquid water at hydrophobic and hydrophilic surfaces - a molecular dynamics simulation study},
213 Volume = {100},
214 Year = {1994},
215 Bdsk-File-1 = {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}}
216
217 @article{Taylor1996,
218 Author = {Ramona S. Taylor and Liem X. Dang and Bruce C. Garrett},
219 Date-Added = {2010-09-08 16:48:01 -0400},
220 Date-Modified = {2010-09-08 16:48:01 -0400},
221 Journal = {J. Phys. Chem.},
222 Keywords = {dewetting; SPC/E},
223 Pages = {11720-11725},
224 Title = {Molecular dynamics simulations of the liquid/vapor interface of SPC/E water},
225 Volume = {100},
226 Year = {1996},
227 Bdsk-File-1 = {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}}
228
229 @article{Du1993,
230 Author = {Q. Du and R. Superfine and E. Freysz and Y.R. Shen},
231 Date-Added = {2010-09-08 16:48:01 -0400},
232 Date-Modified = {2010-09-08 16:48:01 -0400},
233 Journal = {Phys. Rev. Lett.},
234 Keywords = {dewetting; water; experiment; hydrophobic boundary},
235 Month = {April},
236 Number = {15},
237 Pages = {2313-2316},
238 Title = {Vibrational spectroscopy of water at the vapor/water interface},
239 Volume = {70},
240 Year = {1993},
241 Bdsk-File-1 = {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}}
242
243 @article{Li2005,
244 Abstract = {A new approach is developed to study the dynamics of the localized process in solutions and other condensed phase systems. The approach employs a fluctuating elastic boundary (FEB) model which encloses the simulated system in an elastic bag that mimics the effects of the bulk solvent. This alleviates the need for periodic boundary conditions and allows for a reduction in the number of solvent molecules that need to be included in the simulation. The boundary bag is modeled as a mesh of quasi-particles connected by elastic bonds. The FEB model allows for volume and density fluctuations characteristic of the bulk system, and the shape of the boundary fluctuates during the course of the simulation to adapt to the configuration fluctuations of the explicit solute-solvent system inside. The method is applied to the simulation of a Lennard-Jones model of liquid argon. Various structural and dynamical quantities are computed and compared with those obtained from conventional periodic boundary simulations. The agreement between the two is excellent in most cases, thus validating the viability of the FEB method.},
245 Author = {Li, Y. and Krilov, G. and Berne, B.J.},
246 Date-Added = {2010-09-08 16:48:01 -0400},
247 Date-Modified = {2010-09-08 16:48:01 -0400},
248 Journal = {J. Phys. Chem. B},
249 Keywords = {Elastic bag; dewetting},
250 Pages = {463-470},
251 Title = {Elastic bag model for molecular dynamics simulations of solvated systems: Application to liquid argon},
252 Volume = {109},
253 Year = {2005},
254 Bdsk-File-1 = {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}}
255
256 @article{Debenedetti1986,
257 Author = {Debenedetti, P.G.},
258 Date-Added = {2010-09-08 16:48:01 -0400},
259 Date-Modified = {2010-09-08 16:48:01 -0400},
260 Journal = {J. Chem. Phys.},
261 Keywords = {fluctuation dissipation},
262 Month = {February},
263 Number = {3},
264 Pages = {1778-1787},
265 Title = {On the relationship between principal fluctuations and stability coefficients in multicomponent systems},
266 Volume = {84},
267 Year = {1986},
268 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAawAAAAAAawAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+RNEZWJlbmVkZXR0aTE5ODYucGRmAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMIx8bC9AAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAx8b7NAAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIARVNlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6RGViZW5lZGV0dGkxOTg2LnBkZgAADgAoABMARABlAGIAZQBuAGUAZABlAHQAdABpADEAOQA4ADYALgBwAGQAZgAPABIACABTAGUAcgBlAG4AaQB0AHkAEgA8VXNlcnMva3N0b2NrZTEvRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9EZWJlbmVkZXR0aTE5ODYucGRmABMAAS8AABUAAgAP//8AAIAF0hwdHh9YJGNsYXNzZXNaJGNsYXNzbmFtZaMfICFdTlNNdXRhYmxlRGF0YVZOU0RhdGFYTlNPYmplY3RfEDAuLi9Eb2N1bWVudHMvUmVzZWFyY2gvUGFwZXJzL0RlYmVuZWRldHRpMTk4Ni5wZGbSHB0kJaIlIVxOU0RpY3Rpb25hcnkSAAGGoF8QD05TS2V5ZWRBcmNoaXZlcgAIABEAFgAfACgAMgA1ADoAPABFAEsAUgBdAGUAbABvAHEAcwB2AHgAegB8AIYAkwCYAKACUAJSAlcCYAJrAm8CfQKEAo0CwALFAsgC1QLaAAAAAAAAAgEAAAAAAAAAKAAAAAAAAAAAAAAAAAAAAuw=}}
269
270 @article{Bagchi1997,
271 Abstract = {Constant temperature and constant pressure molecular dynamics calculations have been performed on the extended simple point charge (SPC/E) model water to understand the effects of pressure on its structural and dynamical properties. The effect of pressure is to increase the presence of interstitial water molecules, which is shown to be responsible for the experimentally observed increase in the first x-ray diffraction peak and a broadening of the OdOO bond angle distribution. These structural changes lead to weaker hydrogen bonding and the observed minimum in the rotational correlation time as a function of pressure. The weak maximum in the measured translational diffusion coefficient at around 1.5 kbar was not reproduced. The temperature of the density maximum was estimated to occur at 245￿4 K, which suggests that structural changes with increasing pressure and decreasing temperature are not quantitatively reproduced by the SPC/E model. {\copyright} 1997 American Institute of Physics. [S0021-9606(97)51644-8]},
272 Author = {Bagchi, K. and Balasubramanian, S. and Klein, M.L.},
273 Date-Added = {2010-09-08 16:48:01 -0400},
274 Date-Modified = {2010-09-08 16:48:01 -0400},
275 Journal = {J. Chem. Phys.},
276 Keywords = {g(r); SPC/E; pressure},
277 Month = {November},
278 Number = {22},
279 Pages = {8561-8567},
280 Title = {The effects of pressure on structural and dynamical properties of associated liquids: Molecular dynamics calculations for the extended simple point charge model of water},
281 Volume = {20},
282 Year = {1997},
283 Bdsk-File-1 = {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}}
284
285 @article{Minceva-Sukarova1984,
286 Author = {Minceva-Sukarova, B. and Sherman, W.F. and Wilkinson, G.R.},
287 Date-Added = {2010-09-08 16:48:01 -0400},
288 Date-Modified = {2010-09-08 16:48:01 -0400},
289 Journal = {J. Phys. C: Solid State Phys.},
290 Keywords = {ice; structure; pressure},
291 Pages = {5833-5850},
292 Title = {The raman spectra of ice (Ih, II, III, V, VI and IX) as functions of pressure and temperature},
293 Volume = {17},
294 Year = {1984},
295 Bdsk-File-1 = {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}}
296
297 @article{Hummer2000,
298 Author = {G. Hummer and S. Garde and A.E. Garc{\'\i}a and L.R. Pratt},
299 Date-Added = {2010-09-08 16:48:01 -0400},
300 Date-Modified = {2010-09-08 16:48:01 -0400},
301 Journal = {Chemical Physics},
302 Keywords = {interface; hydrophobic boundary; structure},
303 Pages = {349-370},
304 Title = {New perspectives on hydrophobic effects},
305 Volume = {258},
306 Year = {2000},
307 Bdsk-File-1 = {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}}
308
309 @article{Perera1991,
310 Author = {Perera, Lalith and Berkowitz, Max L.},
311 Date-Added = {2010-09-08 16:48:01 -0400},
312 Date-Modified = {2010-09-08 16:48:01 -0400},
313 Journal = {J. Chem. Phys.},
314 Keywords = {ions; polarizable},
315 Month = {August},
316 Number = {3},
317 Pages = {1954-1963},
318 Title = {Many-body effects in molecular dynamics simulations of Na+(H2O)n and Cl-(H2O)n clusters},
319 Volume = {95},
320 Year = {1991},
321 Bdsk-File-1 = {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}}
322
323 @article{Stuart1996,
324 Abstract = {Polarizable and nonpolarizable potential models for both water and chloride are used to address the issue of surfaceVsinteriorsolvationofthechlorideioninCl(H2O)n-clusters,fornupto255. Wefindthat,evenfor the largest clusters, simulations with polarizable water models show that the chloride ion is preferentially solvated near the surface of the cluster. This behavior is not observed with a nonpolarizable model. The many-body effects are not directly responsible for this solvation behavior; polarizability appears to be important primarilyforitsroleinfacilitatingalargeraveragedipolemomentonthewatermodel. Polarizabilityonthe chloride ion is not found to have a substantial effect on the structure of the clusters.},
325 Author = {Stuart, S.J. and Berne, B.J.},
326 Date-Added = {2010-09-08 16:48:01 -0400},
327 Date-Modified = {2010-09-08 16:48:01 -0400},
328 Journal = {J. Phys. Chem.},
329 Keywords = {ions; polarizable; chloride},
330 Pages = {11934-11943},
331 Title = {Effects of polarizability on the hydration of the chloride ion},
332 Volume = {100},
333 Year = {1996},
334 Bdsk-File-1 = {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}}
335
336 @article{Motakabbir1990,
337 Abstract = {Molecular dynamics computer simulations on rigid SPC/E water molecules were performed. The goal of the simulations is to study the behavior of isothermal compressibility, which was calculated in the simulations at T = 298, 273, and 248 K. Thecalculatedisothermalcompressibilitiesatthesetemperaturesdisplayatrendcontrarytotheexperimentalobservations. The hydrogen-bonded network in water was also investigated. No correlation between the temperature dependence of isothermal compressibility and the number of hydrogen-bonded pentagons was observed.},
338 Author = {Motakabbir, K.A. and Berkowitz, M.},
339 Date-Added = {2010-09-08 16:48:01 -0400},
340 Date-Modified = {2010-09-08 16:48:01 -0400},
341 Journal = {J. Phys. Chem.},
342 Keywords = {isothermal compressibility; SPC/E; Pa},
343 Pages = {8359-8362},
344 Title = {Isothermal compressibility of SPC/E water},
345 Volume = {94},
346 Year = {1990},
347 Bdsk-File-1 = {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}}
348
349 @article{Vedamuthu1995,
350 Author = {Vedamuthu, Mary and Singh, Surjit and Robinson, G. Wilse},
351 Date-Added = {2010-09-08 16:48:01 -0400},
352 Date-Modified = {2010-09-08 16:48:01 -0400},
353 Journal = {J. Phys. Chem.},
354 Keywords = {isothermal compressibility; water},
355 Pages = {9263-9267},
356 Title = {Properties of liquid water. 4. The isothermal compressibility minimum near 50 C},
357 Volume = {99},
358 Year = {1995},
359 Bdsk-File-1 = {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}}
360
361 @article{Brancato2009,
362 Author = {Giuseppe Brancato and Nadia Rega and Vincenzo Barone},
363 Date-Added = {2010-09-08 16:48:01 -0400},
364 Date-Modified = {2010-09-08 16:48:01 -0400},
365 Journal = {Chem. Phys. Lett},
366 Keywords = {non-periodic boundary conditions},
367 Pages = {177-181},
368 Title = {Molecular dynamics simulations in a NpT ensemble using non-periodic boundary conditions},
369 Volume = {483},
370 Year = {2009},
371 Bdsk-File-1 = {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}}
372
373 @article{Baltazar2006,
374 Author = {S.E. Baltazar and A.H. Romero and J.L. Rodr{\'\i}guez-L{\'o}pez and H. Terrones and R. Marto{\v n}{\'a}k},
375 Date-Added = {2010-09-08 16:48:01 -0400},
376 Date-Modified = {2010-09-08 16:48:01 -0400},
377 Journal = {Computational Materials Science},
378 Keywords = {NPT},
379 Pages = {526-536},
380 Title = {Assessment of isobaric-isothermal (NPT) simulations for finite systems},
381 Volume = {37},
382 Year = {2006},
383 Bdsk-File-1 = {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}}
384
385 @article{Urquidi1999,
386 Author = {J. Urquidi and S. Singh and C.H. Cho and G.W. Robinson},
387 Date-Added = {2010-09-08 16:48:01 -0400},
388 Date-Modified = {2010-09-08 16:48:01 -0400},
389 Journal = {Phys. Rev. Lett.},
390 Keywords = {pressure; structure},
391 Month = {September},
392 Number = {12},
393 Pages = {2348-2350},
394 Title = {Origin of temperature and pressure effects on the radial distribution function of water},
395 Volume = {83},
396 Year = {1999},
397 Bdsk-File-1 = {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}}
398
399 @article{Robinson1999,
400 Author = {G. Wilse Robinson and Chul Hee Cho and Jacob Urquidi},
401 Date-Added = {2010-09-08 16:48:01 -0400},
402 Date-Modified = {2010-09-08 16:48:01 -0400},
403 Journal = {J. Chem. Phys.},
404 Keywords = {pressure; structure},
405 Month = {July},
406 Number = {2},
407 Pages = {698-702},
408 Title = {Isobestic points in liquid water: Further strong evidence for the two-state mixture model},
409 Volume = {111},
410 Year = {1999},
411 Bdsk-File-1 = {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}}
412
413 @article{Gorbaty1999,
414 Author = {Yu. E. Gorbaty and G.V. Bondarenko and A.G. Kalinichev and A.V. Okhulkov},
415 Date-Added = {2010-09-08 16:48:01 -0400},
416 Date-Modified = {2010-09-08 16:48:01 -0400},
417 Journal = {Mol. Phys.},
418 Keywords = {pressure; structure},
419 Number = {11},
420 Pages = {1659-1665},
421 Title = {The effect of pressure on hydrogen bonding in water: IR study of νOD HDO at pressures of up to 1500 bar},
422 Volume = {96},
423 Year = {1999},
424 Bdsk-File-1 = {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}}
425
426 @article{Stillinger1974,
427 Abstract = {The technique of computer simulation by molecular dynamics has been used to investigate highly compressed water at mass density 1.346 glcm3. The calculations involve 216 rigid molecules, subject to an additive interaction (the "ST2 potential") whose strong anisotropic character has been shown to describe the hydrogen bond phenomenon. In the light of previous calculations on the same model at ordinary pressures, substantial restructuring of the liquid in response to compression is obvious. No evidence arises to support description of the liquid in terms of crystal structures of ices VI and VII, the solid forms that might be expected to be relevant at the chosen density. The calculations indicate that the initial effect of pressure increase (at I atm) leads to increased fluidity, as is known to be the case for real water.},
428 Author = {Frank H. Stillinger and Aneesur Rahman},
429 Date-Added = {2010-09-08 16:48:01 -0400},
430 Date-Modified = {2010-09-08 16:48:01 -0400},
431 Journal = {J. Chem. Phys.},
432 Keywords = {pressure; structure; water},
433 Month = {December},
434 Number = {12},
435 Pages = {4973-4980},
436 Title = {Molecular dynamics study of liquid water under high compression},
437 Volume = {61},
438 Year = {1974},
439 Bdsk-File-1 = {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}}
440
441 @article{Impey1981,
442 Author = {R.W. Impey and M.L. Klein and I.R. McDonald},
443 Date-Added = {2010-09-08 16:48:01 -0400},
444 Date-Modified = {2010-09-08 16:48:01 -0400},
445 Journal = {J. Chem. Phys.},
446 Keywords = {pressure; structure; water},
447 Number = {1},
448 Pages = {647-652},
449 Title = {Molecular dynamics studies of the structure of water at high temperatures and density},
450 Volume = {74},
451 Year = {1981},
452 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAZQAAAAAAZQAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+Q1JbXBleTE5ODEucGRmAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMMyDvSPQAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyDwKfQAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIAP1NlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6SW1wZXkxOTgxLnBkZgAADgAcAA0ASQBtAHAAZQB5ADEAOQA4ADEALgBwAGQAZgAPABIACABTAGUAcgBlAG4AaQB0AHkAEgA2VXNlcnMva3N0b2NrZTEvRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9JbXBleTE5ODEucGRmABMAAS8AABUAAgAP//8AAIAF0hwdHh9YJGNsYXNzZXNaJGNsYXNzbmFtZaMfICFdTlNNdXRhYmxlRGF0YVZOU0RhdGFYTlNPYmplY3RfECouLi9Eb2N1bWVudHMvUmVzZWFyY2gvUGFwZXJzL0ltcGV5MTk4MS5wZGbSHB0kJaIlIVxOU0RpY3Rpb25hcnkSAAGGoF8QD05TS2V5ZWRBcmNoaXZlcgAIABEAFgAfACgAMgA1ADoAPABFAEsAUgBdAGUAbABvAHEAcwB2AHgAegB8AIYAkwCYAKACOAI6Aj8CSAJTAlcCZQJsAnUCogKnAqoCtwK8AAAAAAAAAgEAAAAAAAAAKAAAAAAAAAAAAAAAAAAAAs4=}}
453
454 @article{Wang2006,
455 Author = {Jiyao Wang and Yuqing Deng and Beno{\^\i}t Roux},
456 Date-Added = {2010-09-08 16:48:01 -0400},
457 Date-Modified = {2010-09-08 16:48:01 -0400},
458 Journal = {Biophysical Journal},
459 Keywords = {restraining potential},
460 Month = {October},
461 Pages = {2798-2814},
462 Title = {Absolute binding free energy calculations using molecular dynamics simulations with restraining potentials},
463 Volume = {91},
464 Year = {2006},
465 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAZAAAAAAAZAAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+QxXYW5nMjAwNi5wZGYAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMoyDQhAgAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyDRZQgAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIAPlNlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6V2FuZzIwMDYucGRmAA4AGgAMAFcAYQBuAGcAMgAwADAANgAuAHAAZABmAA8AEgAIAFMAZQByAGUAbgBpAHQAeQASADVVc2Vycy9rc3RvY2tlMS9Eb2N1bWVudHMvUmVzZWFyY2gvUGFwZXJzL1dhbmcyMDA2LnBkZgAAEwABLwAAFQACAA///wAAgAXSHB0eH1gkY2xhc3Nlc1okY2xhc3NuYW1lox8gIV1OU011dGFibGVEYXRhVk5TRGF0YVhOU09iamVjdF8QKS4uL0RvY3VtZW50cy9SZXNlYXJjaC9QYXBlcnMvV2FuZzIwMDYucGRm0hwdJCWiJSFcTlNEaWN0aW9uYXJ5EgABhqBfEA9OU0tleWVkQXJjaGl2ZXIACAARABYAHwAoADIANQA6ADwARQBLAFIAXQBlAGwAbwBxAHMAdgB4AHoAfACGAJMAmACgAjQCNgI7AkQCTwJTAmECaAJxAp0CogKlArICtwAAAAAAAAIBAAAAAAAAACgAAAAAAAAAAAAAAAAAAALJ}}
466
467 @article{Warshel1979,
468 Author = {Warshel, Arieh},
469 Date-Added = {2010-09-08 16:48:01 -0400},
470 Date-Modified = {2010-09-08 16:48:01 -0400},
471 Journal = {J. Phys. Chem.},
472 Keywords = {SCSSD; boundary; water},
473 Number = {12},
474 Pages = {1640-1652},
475 Title = {Calculations of chemical processes in solutions},
476 Volume = {83},
477 Year = {1979},
478 Bdsk-File-1 = {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}}
479
480 @article{Campo2010,
481 Author = {M.G. Campo},
482 Date-Added = {2010-09-08 16:48:01 -0400},
483 Date-Modified = {2010-09-08 16:48:01 -0400},
484 Journal = {Papers in Physics},
485 Keywords = {SPC/E},
486 Number = {article 020001},
487 Pages = {020001-1 - 020001-7},
488 Title = {Structural and dynamic properties of SPC/E water},
489 Volume = {2},
490 Year = {2010},
491 Bdsk-File-1 = {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}}
492
493 @article{Berendsen1987,
494 Author = {H.J.C. Berendsen and J.R. Grigera and T.P. Straatsma},
495 Date-Added = {2010-09-08 16:48:01 -0400},
496 Date-Modified = {2010-09-08 16:48:01 -0400},
497 Journal = {J. Phys. Chem.},
498 Keywords = {SPC/E},
499 Pages = {6269-6271},
500 Title = {The missing term in effective pair potentials},
501 Volume = {91},
502 Year = {1987},
503 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAaQAAAAAAaQAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+RFCZXJlbmRzZW4xOTg3LnBkZgAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMcyCrIgAAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyCsAwAAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIAQ1NlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6QmVyZW5kc2VuMTk4Ny5wZGYAAA4AJAARAEIAZQByAGUAbgBkAHMAZQBuADEAOQA4ADcALgBwAGQAZgAPABIACABTAGUAcgBlAG4AaQB0AHkAEgA6VXNlcnMva3N0b2NrZTEvRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9CZXJlbmRzZW4xOTg3LnBkZgATAAEvAAAVAAIAD///AACABdIcHR4fWCRjbGFzc2VzWiRjbGFzc25hbWWjHyAhXU5TTXV0YWJsZURhdGFWTlNEYXRhWE5TT2JqZWN0XxAuLi4vRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9CZXJlbmRzZW4xOTg3LnBkZtIcHSQloiUhXE5TRGljdGlvbmFyeRIAAYagXxAPTlNLZXllZEFyY2hpdmVyAAgAEQAWAB8AKAAyADUAOgA8AEUASwBSAF0AZQBsAG8AcQBzAHYAeAB6AHwAhgCTAJgAoAJIAkoCTwJYAmMCZwJ1AnwChQK2ArsCvgLLAtAAAAAAAAACAQAAAAAAAAAoAAAAAAAAAAAAAAAAAAAC4g==}}
504
505 @article{Jorgensen1998,
506 Abstract = {Monte Carlo statistical mechanics simulations have been carried out with the TIP3P, SPC, and TIP4P models for liquid water at 13 temperatures from 􏰮50􏰯C to 100􏰯C at 1 atm. Long runs with 512 water molecules provided definitive results for densities. Although the TIP4P model yields a flat region in the density profile and a temperature of maximum density near 􏰮15􏰯C, the SPC and TIP3P models show monotonically increasing density with decreasing temperature. Results for heats of vaporization, isothermal compressibilities, and coefficients of thermal expansion and their convergence characteristics are also reported. 􏰱 1998 John Wiley & Sons, Inc. J Comput Chem 19: 1179􏰰1186, 1998},
507 Author = {Jorgensen, W.L. and Jenson, C.},
508 Date-Added = {2010-09-08 16:48:01 -0400},
509 Date-Modified = {2010-09-08 16:48:01 -0400},
510 Journal = {Journal of Computational Chemistry},
511 Keywords = {SPC/E; density; water models; structure; g(r)},
512 Number = {10},
513 Pages = {1179-1186},
514 Title = {Temperature dependence of TIP3P, SPC, and TIP4P water from NPT Monte Carlo simulations: Seeking temperatures of maximum density},
515 Volume = {19},
516 Year = {1998},
517 Bdsk-File-1 = {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}}
518
519 @article{Peltz2003,
520 Author = {Csaba Peltz and Andr{\'a}s Baranyai and Ariel A. Chialvo and Peter T. Cummings},
521 Date-Added = {2010-09-08 16:48:01 -0400},
522 Date-Modified = {2010-09-08 16:48:01 -0400},
523 Journal = {Molecular Simulation},
524 Keywords = {SPC/E; structure},
525 Number = {1},
526 Pages = {13-21},
527 Title = {Microstructure of water at the level of three-particle correlation functions as predicted by classical intermolecular models},
528 Volume = {29},
529 Year = {2003},
530 Bdsk-File-1 = {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}}
531
532 @article{Kratky1980,
533 Author = {K.W. Kratky},
534 Date-Added = {2010-09-08 16:48:01 -0400},
535 Date-Modified = {2010-09-08 16:48:01 -0400},
536 Journal = {Journal of Computational Physics},
537 Keywords = {spherical boundary conditions},
538 Pages = {205-217},
539 Title = {New boundary conditions for computer experiments of thermodynamic systems},
540 Volume = {37},
541 Year = {1980},
542 Bdsk-File-1 = {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}}
543
544 @article{Kratky1982,
545 Author = {K.W. Kratky and W. Schreiner},
546 Date-Added = {2010-09-08 16:48:01 -0400},
547 Date-Modified = {2010-09-08 16:48:01 -0400},
548 Journal = {J. Chem. Phys.},
549 Keywords = {spherical boundary conditions},
550 Pages = {313-320},
551 Title = {Computational techniques for spherical boundary conditions},
552 Volume = {47},
553 Year = {1982},
554 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAZgAAAAAAZgAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+Q5LcmF0a3kxOTgyLnBkZgAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMmyDQQ7gAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyDRJLgAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIAQFNlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6S3JhdGt5MTk4Mi5wZGYADgAeAA4ASwByAGEAdABrAHkAMQA5ADgAMgAuAHAAZABmAA8AEgAIAFMAZQByAGUAbgBpAHQAeQASADdVc2Vycy9rc3RvY2tlMS9Eb2N1bWVudHMvUmVzZWFyY2gvUGFwZXJzL0tyYXRreTE5ODIucGRmAAATAAEvAAAVAAIAD///AACABdIcHR4fWCRjbGFzc2VzWiRjbGFzc25hbWWjHyAhXU5TTXV0YWJsZURhdGFWTlNEYXRhWE5TT2JqZWN0XxArLi4vRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9LcmF0a3kxOTgyLnBkZtIcHSQloiUhXE5TRGljdGlvbmFyeRIAAYagXxAPTlNLZXllZEFyY2hpdmVyAAgAEQAWAB8AKAAyADUAOgA8AEUASwBSAF0AZQBsAG8AcQBzAHYAeAB6AHwAhgCTAJgAoAI8Aj4CQwJMAlcCWwJpAnACeQKnAqwCrwK8AsEAAAAAAAACAQAAAAAAAAAoAAAAAAAAAAAAAAAAAAAC0w==}}
555
556 @article{Schreiner1983,
557 Author = {W. Schreiner and K.W. Kratky},
558 Date-Added = {2010-09-08 16:48:01 -0400},
559 Date-Modified = {2010-09-08 16:48:01 -0400},
560 Journal = {Mol. Phys.},
561 Keywords = {spherical boundary conditions},
562 Number = {3},
563 Pages = {435-452},
564 Title = {Finiteness effects in computer simulation of fluids with spherical boundary conditions},
565 Volume = {50},
566 Year = {1983},
567 Bdsk-File-1 = {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}}
568
569 @article{Brooks1983a,
570 Author = {Brooks, C.L III and Karplus, M.},
571 Date-Added = {2010-09-08 16:48:01 -0400},
572 Date-Modified = {2010-09-08 16:48:38 -0400},
573 Journal = {J. Chem. Phys.},
574 Keywords = {stochastic boundary conditions},
575 Month = {December},
576 Number = {12},
577 Pages = {6312-6325},
578 Title = {Deformable stochastic boundaries in molecular dynamics},
579 Volume = {79},
580 Year = {1983},
581 Bdsk-File-1 = {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}}
582
583 @article{Berkowitz1982,
584 Author = {Max Berkowitz and J. Andrew McCammon},
585 Date-Added = {2010-09-08 16:48:01 -0400},
586 Date-Modified = {2010-09-08 16:48:01 -0400},
587 Journal = {Chem. Phys. Lett.},
588 Keywords = {stochastic boundary conditions},
589 Month = {July},
590 Number = {3},
591 Pages = {215-217},
592 Title = {Molecular dynamics with stochastic boundary conditions},
593 Volume = {90},
594 Year = {1982},
595 Bdsk-File-1 = {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}}
596
597 @article{Paolantoni2009,
598 Author = {M. Paolantoni and N. Faginas Lago and M. Albert{\'\i} and A. Lagan{\'a}},
599 Date-Added = {2010-09-08 16:48:01 -0400},
600 Date-Modified = {2010-09-08 16:48:01 -0400},
601 Journal = {J. Phys. Chem. A},
602 Keywords = {tetrahedrality, q},
603 Pages = {15100-15105},
604 Title = {Tetrahedral ordering in water: Raman profiles and their temperature dependence},
605 Volume = {113},
606 Year = {2009},
607 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAagAAAAAAagAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+RJQYW9sYW50b25pMjAwOS5wZGYAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMeyGSd7gAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyGTWLgAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIARFNlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6UGFvbGFudG9uaTIwMDkucGRmAA4AJgASAFAAYQBvAGwAYQBuAHQAbwBuAGkAMgAwADAAOQAuAHAAZABmAA8AEgAIAFMAZQByAGUAbgBpAHQAeQASADtVc2Vycy9rc3RvY2tlMS9Eb2N1bWVudHMvUmVzZWFyY2gvUGFwZXJzL1Bhb2xhbnRvbmkyMDA5LnBkZgAAEwABLwAAFQACAA///wAAgAXSHB0eH1gkY2xhc3Nlc1okY2xhc3NuYW1lox8gIV1OU011dGFibGVEYXRhVk5TRGF0YVhOU09iamVjdF8QLy4uL0RvY3VtZW50cy9SZXNlYXJjaC9QYXBlcnMvUGFvbGFudG9uaTIwMDkucGRm0hwdJCWiJSFcTlNEaWN0aW9uYXJ5EgABhqBfEA9OU0tleWVkQXJjaGl2ZXIACAARABYAHwAoADIANQA6ADwARQBLAFIAXQBlAGwAbwBxAHMAdgB4AHoAfACGAJMAmACgAkwCTgJTAlwCZwJrAnkCgAKJArsCwALDAtAC1QAAAAAAAAIBAAAAAAAAACgAAAAAAAAAAAAAAAAAAALn}}
608
609 @article{Chau1998,
610 Author = {P.L. Chau and A.J. Hardwick},
611 Date-Added = {2010-09-08 16:48:01 -0400},
612 Date-Modified = {2010-09-08 16:48:01 -0400},
613 Journal = {Mol. Phys.},
614 Keywords = {tetrahedrality; q; structure},
615 Number = {3},
616 Pages = {511-518},
617 Title = {A new order parameter for tetrahedral configurations},
618 Volume = {93},
619 Year = {1998},
620 Bdsk-File-1 = {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}}
621
622 @article{Scatena2001,
623 Author = {Scatena, L.F. and Brown, M.G. and Richmond, G.L.},
624 Date-Added = {2010-09-08 16:48:01 -0400},
625 Date-Modified = {2010-09-08 16:48:01 -0400},
626 Journal = {Science},
627 Keywords = {water; experiment; dewetting; hydrophobic boundary},
628 Month = {May},
629 Pages = {908-912},
630 Title = {Water at hydrophobic surfaces: Weak hydrogen bonding and strong orientation effects},
631 Volume = {292},
632 Year = {2001},
633 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAZwAAAAAAZwAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+Q9TY2F0ZW5hMjAwMS5wZGYAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMDyCQtvwAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyCRl/wAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIAQVNlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6U2NhdGVuYTIwMDEucGRmAAAOACAADwBTAGMAYQB0AGUAbgBhADIAMAAwADEALgBwAGQAZgAPABIACABTAGUAcgBlAG4AaQB0AHkAEgA4VXNlcnMva3N0b2NrZTEvRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9TY2F0ZW5hMjAwMS5wZGYAEwABLwAAFQACAA///wAAgAXSHB0eH1gkY2xhc3Nlc1okY2xhc3NuYW1lox8gIV1OU011dGFibGVEYXRhVk5TRGF0YVhOU09iamVjdF8QLC4uL0RvY3VtZW50cy9SZXNlYXJjaC9QYXBlcnMvU2NhdGVuYTIwMDEucGRm0hwdJCWiJSFcTlNEaWN0aW9uYXJ5EgABhqBfEA9OU0tleWVkQXJjaGl2ZXIACAARABYAHwAoADIANQA6ADwARQBLAFIAXQBlAGwAbwBxAHMAdgB4AHoAfACGAJMAmACgAkACQgJHAlACWwJfAm0CdAJ9AqwCsQK0AsECxgAAAAAAAAIBAAAAAAAAACgAAAAAAAAAAAAAAAAAAALY}}
634
635 @article{Vega2005,
636 Abstract = {The melting point of ice Ih for the TIP3P, SPC, SPC/E, TIP4P, TIP4P/Ew and TIP5P models has been determined by computer simulation. It has been found that the melting points of ice Ih for these models are 146, 190, 215, 232, 245 and 274 K respectively. Thus from the models of water available so far only TIP5P reproduces the experimental melting point of water. The relative stability of ice II with respect to ice Ih at the normal melting point has also been considered. Ice II is more stable than ice Ih for the TIP3P, SPC, SPC/E and TIP5P models. Only for the TIP4P and TIP4P/Ew models is ice Ih more stable than ice II at low pressures. The complete phase diagram for the SPC/E, TIP4P and TIP5P models has been computed. It has been found that SPC/E and TIP5P do not correctly describe the phase diagram of water. However, TIP4P provides a qualitatively correct description of the phase diagram of water. A slight modification of the parameters of the TIP4P model yields a new model, denoted as TIP4P/ice, which reproduces the experimental melting point of water and provides an excellent description of the densities of all ice phases.},
637 Author = {Vega, C. and Abascal, J.L.F. and MacDowell, L.G. and McBride, C.},
638 Date-Added = {2010-09-08 16:48:01 -0400},
639 Date-Modified = {2010-09-08 16:48:01 -0400},
640 Journal = {J. Phys.: Condes. Matter},
641 Keywords = {water; model},
642 Pages = {S3283-S3288},
643 Title = {Can simple models describe the phase diagram of water?},
644 Volume = {17},
645 Year = {2005},
646 Bdsk-File-1 = {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}}
647
648 @article{Jhon2006,
649 Author = {Jhon, Young In and No, Kyoung Tai and Jhon, Mu Shik},
650 Date-Added = {2010-09-08 16:48:01 -0400},
651 Date-Modified = {2010-09-08 16:48:01 -0400},
652 Journal = {Fluid Phase Equilibria},
653 Keywords = {water; q; tetrahedrality},
654 Pages = {160-166},
655 Title = {The molecular-level relationship between the properties of liquid water molecules and orientational order},
656 Volume = {244},
657 Year = {2006},
658 Bdsk-File-1 = {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}}
659
660 @article{Ohtaki1997,
661 Author = {Hitoshi Ohtaki and Tam{\'a}s Radnai and Toshio Yamaguchi},
662 Date-Added = {2010-09-08 16:48:01 -0400},
663 Date-Modified = {2010-09-08 16:48:01 -0400},
664 Journal = {Chemical Society Reviews},
665 Keywords = {water; structure},
666 Pages = {41-51},
667 Title = {Structure of water under subcritical and supercritical conditions studied by solution X-ray diffraction},
668 Year = {1997},
669 Bdsk-File-1 = {YnBsaXN0MDDUAQIDBAUIJidUJHRvcFgkb2JqZWN0c1gkdmVyc2lvblkkYXJjaGl2ZXLRBgdUcm9vdIABqAkKFRYXGyIjVSRudWxs0wsMDQ4RFFpOUy5vYmplY3RzV05TLmtleXNWJGNsYXNzog8QgASABqISE4ACgAOAB1lhbGlhc0RhdGFccmVsYXRpdmVQYXRo0hgNGRpXTlMuZGF0YU8RAZgAAAAAAZgAAgAACFNlcmVuaXR5AAAAAAAAAAAAAAAAAAAAAAAAAMiiw+JIKwAAABJC+Q5PaHRha2kxOTk3LnBkZgAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAEkMGyDvR8gAAAAAAAAAAAAEABAAACSAAAAAAAAAAAAAAAAAAAAAGUGFwZXJzABAACAAAyKL8IgAAABEACAAAyDwKMgAAAAEAFAASQvkAEkLjABI4nQASOJAAAJHaAAIAQFNlcmVuaXR5OlVzZXJzOmtzdG9ja2UxOkRvY3VtZW50czpSZXNlYXJjaDpQYXBlcnM6T2h0YWtpMTk5Ny5wZGYADgAeAA4ATwBoAHQAYQBrAGkAMQA5ADkANwAuAHAAZABmAA8AEgAIAFMAZQByAGUAbgBpAHQAeQASADdVc2Vycy9rc3RvY2tlMS9Eb2N1bWVudHMvUmVzZWFyY2gvUGFwZXJzL09odGFraTE5OTcucGRmAAATAAEvAAAVAAIAD///AACABdIcHR4fWCRjbGFzc2VzWiRjbGFzc25hbWWjHyAhXU5TTXV0YWJsZURhdGFWTlNEYXRhWE5TT2JqZWN0XxArLi4vRG9jdW1lbnRzL1Jlc2VhcmNoL1BhcGVycy9PaHRha2kxOTk3LnBkZtIcHSQloiUhXE5TRGljdGlvbmFyeRIAAYagXxAPTlNLZXllZEFyY2hpdmVyAAgAEQAWAB8AKAAyADUAOgA8AEUASwBSAF0AZQBsAG8AcQBzAHYAeAB6AHwAhgCTAJgAoAI8Aj4CQwJMAlcCWwJpAnACeQKnAqwCrwK8AsEAAAAAAAACAQAAAAAAAAAoAAAAAAAAAAAAAAAAAAAC0w==}}
670
671 @article{Tanaka1987,
672 Author = {Hideki Tanaka and Iwao Ohmine},
673 Date-Added = {2010-09-08 16:48:01 -0400},
674 Date-Modified = {2010-09-08 16:48:01 -0400},
675 Journal = {J. Chem. Phys.},
676 Keywords = {water; structure},
677 Number = {10},
678 Pages = {6128-6139},
679 Title = {Large local energy fluctuations in water},
680 Volume = {87},
681 Year = {1987},
682 Bdsk-File-1 = {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}}
683
684 @article{Kalinichev1999,
685 Abstract = {Monte Carlo computer simulations with the TIP4P intermolecular potential are performed in 9 thermodynamic states of compressed liquid water along the 298 K isotherm. Two distinct pressure ranges are found in the pressure dependence of the O-O near-neighbor distances in qualitative agreement with the X-ray diffraction data. Nevertheless, the experimentally observed minimum in this dependence is not reproduced by the present simulations. The evolution of hydrogen-bonded network in liquid water under gradual compression is quantitatively analyzed using the combined geometric and energetic criterion of hydrogen bonding. Despite some bending and weakening of the existing hydrogen bonds, the average topology of the H-bonded network remains intact, and the average number of hydrogen bonds per a water molecule remains constant ((nrm) = 3.2) over the whole pressure range studied, while the increase in density is mainly achieved by an increased packing efficiency of non-bonded nearest and second nearest neighbors.},
686 Author = {Kalinichev, A.G. and Gorbaty, Yu.E. and Okhulkov, A.V.},
687 Date-Added = {2010-09-08 16:48:01 -0400},
688 Date-Modified = {2010-09-08 16:48:01 -0400},
689 Journal = {Journal of Molecular Liquids},
690 Keywords = {water; structure; g(r); pressure; TIP4P},
691 Pages = {57-72},
692 Title = {Structure and hydrogen bonding of liquid water at high hydrostatic pressures: Monte Carlo NPT-ensemble simulations up to 10 kbar},
693 Volume = {82},
694 Year = {1999},
695 Bdsk-File-1 = {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}}
696
697 @article{Mishima1998,
698 Author = {Osamu Mishima and H. Eugene Stanley},
699 Date-Added = {2010-09-08 16:48:01 -0400},
700 Date-Modified = {2010-09-08 16:48:01 -0400},
701 Journal = {Nature},
702 Keywords = {water; structure; liquid-liquid transition},
703 Month = {March},
704 Pages = {164-168},
705 Title = {Decompression-induced melting of ice IV and the liquid-liquid transition in water},
706 Volume = {392},
707 Year = {1998},
708 Bdsk-File-1 = {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}}
709
710 @article{Jancso1984,
711 Abstract = {Molecular dynamics simulations of liquid water at densities of 0.9718 and 1.346 g/cm3. and at temperatures of 63 and 77'T have been performed employing a modified version of the central-force model of water. The structural changes observed are in reasonably good agreement with recent high-pressure neutron scattering studies. The self-diffusion coefficient has been found to decrease by = 35% on compression. The OH stretching frequency underwent a shift of 10 cm-' in the directionof lower frequencies and was accompanied by an increase in the average O-H bond length.},
712 Author = {Jancs{\'o}, G. and Bopp, P. and Heinzinger, K.},
713 Date-Added = {2010-09-08 16:48:01 -0400},
714 Date-Modified = {2010-09-08 16:48:01 -0400},
715 Journal = {Chemical Physics},
716 Keywords = {water; structure; pressure},
717 Pages = {377-387},
718 Title = {Molecular dynamics study of high-density liquid water using a modified central-force potential},
719 Volume = {85},
720 Year = {1984},
721 Bdsk-File-1 = {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}}
722
723 @article{Kumar,
724 Author = {Pradeep Kumar and Sergey V. Buldyrev and H. Eugene Stanley},
725 Date-Added = {2010-09-08 16:48:01 -0400},
726 Date-Modified = {2010-09-08 16:48:01 -0400},
727 Journal = {arXiv:0807.4699v1},
728 Keywords = {water; structure; q; tetrahedrality},
729 Title = {Space-Time Correlations in the Orientational Order Parameter and the Orientational Entropy of Water},
730 Bdsk-File-1 = {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}}
731
732 @article{Errington2001,
733 Author = {Jeffrey R. Errington and Pablo G. Debenedetti},
734 Date-Added = {2010-09-08 16:48:01 -0400},
735 Date-Modified = {2010-09-08 16:48:01 -0400},
736 Journal = {Nature},
737 Keywords = {water; structure; q; tetrahedrality},
738 Month = {January},
739 Pages = {318-321},
740 Title = {Relationship between structural order and the anomalies of liquid water},
741 Volume = {409},
742 Year = {2001},
743 Bdsk-File-1 = {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}}
744
745 @article{cite-key,
746 Date-Added = {2010-08-27 15:57:54 -0400},
747 Date-Modified = {2010-08-27 15:57:54 -0400}}
748
749 @article{Glattli2002,
750 Author = {A. Gl{\"a}ttli and X. Daura and W.F. van Gunsteren},
751 Date-Added = {2010-08-27 15:54:36 -0400},
752 Date-Modified = {2010-08-27 15:57:25 -0400},
753 Journal = {J. Chem. Phys.},
754 Keywords = {isothermal compressibility; SPC/E, atm},
755 Month = {June},
756 Number = {22},
757 Pages = {9811-9828},
758 Title = {Derivation of an improved single point charge model for liquid water: SPC/A and SPC/L},
759 Volume = {116},
760 Year = {2002}}
761
762 @article{Jeffrey:2006dk,
763 Author = {Jeffrey,D. J. and Onishi,Y.},
764 Date-Added = {2008-04-30 12:15:31 -0400},
765 Date-Modified = {2008-04-30 12:15:31 -0400},
766 Journal = {Journal of Fluid Mechanics Digital Archive},
767 M3 = {10.1017/S0022112084000355},
768 Number = {-1},
769 Pages = {261--290},
770 Title = {Calculation of the resistance and mobility functions for two unequal rigid spheres in low-Reynolds-number flow},
771 Ty = {JOUR},
772 Volume = {139},
773 Year = {2006}}
774
775 @article{Goldman:1966ph,
776 Abstract = { Bipolar coordinates are employed to determine the terminal settling motion of two, identical, homogeneous, unconstrained spheres in an unbounded fluid at small Reynolds numbers. Exact numerical values are obtained for the linear and angular velocities of the spheres as a function of their relative separation and of the orientation of their line-of-centers relative to the direction of gravity. Comparison with published experimental data indicates good agreement, especially when wall effects are taken into account.},
777 Author = {Goldman, A. J. and Cox, R. G. and Brenner, H.},
778 Date-Added = {2008-04-30 12:12:54 -0400},
779 Date-Modified = {2008-04-30 12:12:54 -0400},
780 Journal = {Chemical Engineering Science},
781 Number = {12},
782 Pages = {1151--1170},
783 Title = {The slow motion of two identical arbitrarily oriented spheres through a viscous fluid},
784 Ty = {JOUR},
785 Url = {http://www.sciencedirect.com/science/article/B6TFK-44360XJ-D0/1/c14cf5c48fab65f0aaa096e60d15fa87},
786 Volume = {21},
787 Year = {1966},
788 Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/B6TFK-44360XJ-D0/1/c14cf5c48fab65f0aaa096e60d15fa87}}
789
790 @article{Brenner:1972th,
791 Abstract = { A general theory is presented for determining the quasistatic Stokes resistance of a particle or an aggregate of particles of arbitrary shape which move with arbitrary translational and rotational velocities in an infinite viscous fluid subjected to a general linear shear flow in the absence of the particles. It is shown that the hydrodynamic resistance of the particles may be characterized by two intrinsic matrices-the grand resistance matrix and the shear resistance matrix, the elements of each matrix being dependent only upon the instantaneous geometrical configuration of the multiparticle system. Explicit expressions for these matrix elements are given for a single ellipsoidal particle and for two spheres. Analytical, closed-form expressions are given for the case where the spheres are widely spaced compared with their radii. When the separation between the spheres is arbitrary, the matrix elements are only determinate numerically for specified ratios of sphere radii and center-to-center separation distances. These numerical values are derived from available bipolar-coordinate system solutions for two spheres. Besides providing a compact and systematic representation of the intrinsic Stokes resistance of multiparticle systems subjected to shear, which does not depend upon the precise velocities of the particles or on the nature of the shear flow, it is demonstrated (by way of example) that the matrix representation permits an immediate determination of the translational and rotational velocities of the individual particles in a neutrally buoyant multiparticle system.},
792 Author = {Brenner, Howard and O'Neill, Michael E.},
793 Date-Added = {2008-04-30 12:12:49 -0400},
794 Date-Modified = {2008-04-30 12:12:49 -0400},
795 Journal = {Chemical Engineering Science},
796 Number = {7},
797 Pages = {1421--1439},
798 Title = {On the Stokes resistance of multiparticle systems in a linear shear field},
799 Ty = {JOUR},
800 Url = {http://www.sciencedirect.com/science/article/B6TFK-444GW12-16J/1/ba6bda9d1e50c88fea6cd92aac2f6bd7},
801 Volume = {27},
802 Year = {1972},
803 Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/B6TFK-444GW12-16J/1/ba6bda9d1e50c88fea6cd92aac2f6bd7}}
804
805 @article{GarciadelaTorreJjp0647941,
806 Affiliation = {Departamento de Qu{\'\i}mica F{\'\i}sica, Facultad de Qu{\'\i}mica, Universidad de Murcia, 30071 Murcia, Spain},
807 Author = {{Garc\'{i}a de la Torre}, Jose and del Rio Echenique, G. and Ortega, A.},
808 Date-Added = {2008-04-30 10:14:50 -0400},
809 Date-Modified = {2008-04-30 10:14:50 -0400},
810 Issn = {1520-6106},
811 Journal = jpcb,
812 Number = {5},
813 Pages = {955-961},
814 Title = {Improved Calculation of Rotational Diffusion and Intrinsic Viscosity of Bead Models for Macromolecules and Nanoparticles},
815 Url = {http://pubs3.acs.org/acs/journals/doilookup?in_doi=10.1021/jp0647941},
816 Volume = {111},
817 Year = {2007},
818 Bdsk-Url-1 = {http://pubs3.acs.org/acs/journals/doilookup?in_doi=10.1021/jp0647941}}
819
820 @article{Garcia-de-la-Torre:2001wd,
821 Abstract = { The calculation of hydrodynamic and other solution properties of rigid macromolecules, using bead-shell model methodologies, requires the specification of the macromolecular shape in a format that can be interfaced with existing programs for hydrodynamic computations. Here, a procedure is presented for such a structural specification that is applicable to arbitrarily shaped particles. A computer program (), in which the user inserts the code needed to determine the structure, produces an structural file that is interpreted by another program () which is in charge of the computation of properties. As simple and yet illustrative examples we consider two cases: (1) dimeric structures composed of ellipsoidal subunits; and (2) toroidal structures, presenting simple equations that predict the properties of toroids with varying radial ratios.},
822 Author = {{Garc\'{i}a de la Torre}, Jose},
823 Date-Added = {2008-04-29 15:11:32 -0400},
824 Date-Modified = {2008-04-29 15:11:32 -0400},
825 Journal = {Biophysical Chemistry},
826 Keywords = {Rigid macromolecules; Hydrodynamic properties; Bead-shell model; Three-dimensional structure},
827 Number = {3},
828 Pages = {265--274},
829 Title = {Building hydrodynamic bead-shell models for rigid bioparticles of arbitrary shape},
830 Ty = {JOUR},
831 Url = {http://www.sciencedirect.com/science/article/B6TFB-44XJKW6-8/1/376af59f3b89aecd8486b1c6186b0953},
832 Volume = {94},
833 Year = {2001},
834 Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/B6TFB-44XJKW6-8/1/376af59f3b89aecd8486b1c6186b0953}}
835
836 @article{Peters:1999uq,
837 Abstract = {The Fokker-Planck (FP) equation describing the dynamics of a single Brownian particle near a fixed external surface is derived using the multiple-time-scales perturbation method, previously used by Cukier and Deutch and Nienhuis in the absence of any external surfaces, and Piasecki ei LII. for two Brownian spheres in a hard fluid. The FP equation includes an explicit expression for the (time-independent) particle friction tensor in terms of the force autocorrelation Function and equilibrium average force on the particle by the surrounding fluid and in the presence of a fixed external surface. such as an adsorbate. The scaling and perturbation analysis given here also shows that the Force autocorrelation function must decay rapidly on the zeroth-order time scale tau(0), which physically requires N-Kn much less than 1, where N-Kn is the Knudsen number (ratio of the length scale for fluid intermolecular interactions to the Brownian particle length scale). This restricts the theory given here to liquid systems where N-Kn much less than 1. For a specified particle configuration with respect to the external surface, equilibrium canonical molecular dynamics (MD) calculations are conducted, as shown here, in order to obtain numerical values of the friction tensor from the force autocorrelation expression. Molecular dynamics computations of the friction tensor for a single spherical particle in the absence of a fixed external surface are shown to recover Stokes' law for various types of fluid molecule-particle interaction potentials. Analytical studies of the static force correlation function also demonstrate the remarkable principle of force-time parity whereby the particle friction coefficient is nearly independent of the fluid molecule-particle interaction potential. Molecular dynamics computations of the friction tensor for a single spherical particle near a fixed external spherical surface (adsorbate) demonstrate a breakdown in continuum hydrodynamic results at close particle surface separation distances on the order of several molecular diameters.},
838 Author = {Peters, MH},
839 Date-Added = {2008-03-13 16:54:59 -0400},
840 Date-Modified = {2008-03-13 16:56:54 -0400},
841 Journal = {Journal of Statistical Physics},
842 Keywords = {Brownian particle; Fokker Planck equation; adsorption; molecular friction; force autocorrelation function; molecular dynamics},
843 Pages = {557-586},
844 Timescited = {0},
845 Title = {Fokker-Planck equation, molecular friction, and molecular dynamics for Brownian particle transport near external solid surfaces},
846 Volume = {94},
847 Year = {1999}}
848
849 @article{Peters:1999qy,
850 Abstract = {The Fokker-Planck equation and molecular-based grand friction tensor are derived for the problem of rotational and translational motions of a structured Brownian particle, including the presence of a structured wall. Using the method of multiple time scales, it is shown that the time independent, grand friction tensor for the Brownian particle includes, in a general way, terms that account fur the fluid molecular mediated interactions with the wall. The resulting Fokker-Planck equation has important applications in processes involving site-specific adsorption of macromolecules, such as affinity chromotography, biological separations, and numerous cellular processes involving attachment of macromolecules. (C) 1999 American Institute of Physics. [S0021-9606(98)51748-5].},
851 Author = {Peters, MH},
852 Date-Added = {2008-03-13 16:54:59 -0400},
853 Date-Modified = {2008-03-13 16:56:44 -0400},
854 Journal = jcp,
855 Pages = {528-538},
856 Timescited = {0},
857 Title = {Fokker-Planck equation and the grand molecular friction tensor for coupled rotational and translational motions of structured Brownian particles near structured surfaces},
858 Volume = {110},
859 Year = {1999}}
860
861 @article{Peters:2000fk,
862 Abstract = {Beginning with the molecular-based Fokker-Planck equation obtained previously [M. H. Peters, J. Chem. Phys. 110, 528 (1999); J. Stat. Phys. 94, 557 (1999)], the Smoluchowski diffusion equation is derived here to describe the spatial and orientational dynamics of molecularly structured macromolecules near molecularly structured surfaces. The formal scaling and perturbation methods employed allow the establishment of definite limits on the use of the Smoluchowski equation when surfaces are present. It is shown that the Smoluchowski equation reduces to that given previously [D. W. Condiff and J. S. Dahler, J. Chem. Phys. 44, 3988 (1966)] in the absence of external surfaces. A specific example application is given involving a spherical macromolecule with electrostatic charge segments near a planar surface with an arbitrary charge distribution. Finally, we show that the short-time solution to the Smoluchowski equation obtained here yields a Brownian dynamics method consistent with that given previously [E. Dickinson, S. A. Allison, and J. A. McCammon, J. Chem. Soc. Faraday Trans. 2 81, 591 (1985)] for orientable, interacting Brownian particles. This study has applications to problems involving site-specific adsorption of orientable, structured Brownian particles, such as association or adsorption of biological macromolecules to cellular surfaces and enzyme-substrate docking kinetics, to name a few. (C) 2000 American Institute of Physics. [S0021-9606(00)50112-3].},
863 Author = {Peters, MH},
864 Date-Added = {2008-03-13 16:54:59 -0400},
865 Date-Modified = {2008-03-13 16:56:20 -0400},
866 Journal = jcp,
867 Pages = {5488-5498},
868 Timescited = {0},
869 Title = {The Smoluchowski diffusion equation for structured macromolecules near structured surfaces},
870 Volume = {112},
871 Year = {2000}}
872
873 @article{Nienhuis:1970lr,
874 Abstract = { A quantummechanical system consisting of N light bath particles and one heavy Brownian linear rotator is considered. By employing the multiple time scale technique and the Wigner representation of quantummechanics, a Fokker-Planck equation for the motion of the Brownian particle is derived. Some properties of this equation are briefly discussed.},
875 Author = {Nienhuis, G.},
876 Date-Added = {2008-03-13 16:53:44 -0400},
877 Date-Modified = {2008-03-13 16:53:44 -0400},
878 Journal = {Physica},
879 Number = {1},
880 Pages = {26--48},
881 Title = {On the microscopic theory of Brownian motion with a rotational degree of freedom},
882 Ty = {JOUR},
883 Url = {http://www.sciencedirect.com/science/article/B6X42-46D224N-BW/2/0e1b39b5a20e979c5fa5e1f560de6413},
884 Volume = {49},
885 Year = {1970},
886 Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/B6X42-46D224N-BW/2/0e1b39b5a20e979c5fa5e1f560de6413}}
887
888 @article{SunX._jp0762020,
889 Affiliation = {Department of Chemistry and Biochemistry, University of Notre Dame, Notre Dame, Indiana 46556},
890 Author = {Sun, X. and Gezelter, J.D.},
891 Date-Added = {2008-02-15 13:48:18 -0500},
892 Date-Modified = {2008-02-15 13:48:18 -0500},
893 Issn = {1520-6106},
894 Journal = jpcb,
895 Number = {7},
896 Pages = {1968-1975},
897 Title = {Dipolar Ordering in the Ripple Phases of Molecular-Scale Models of Lipid Membranes},
898 Url = {http://pubs3.acs.org/acs/journals/doilookup?in_doi=10.1021/jp0762020},
899 Volume = {112},
900 Year = {2008},
901 Bdsk-Url-1 = {http://pubs3.acs.org/acs/journals/doilookup?in_doi=10.1021/jp0762020}}
902
903 @book{Schlick2002,
904 Address = {Secaucus, NJ, USA},
905 Author = {Tamar Schlick},
906 Date-Added = {2008-02-12 16:52:19 -0500},
907 Date-Modified = {2008-02-12 16:53:15 -0500},
908 Isbn = {038795404X},
909 Publisher = {Springer-Verlag New York, Inc.},
910 Title = {Molecular Modeling and Simulation: An Interdisciplinary Guide},
911 Year = {2002}}
912
913 @article{Chun:2000fj,
914 Abstract = {A modeling approach that can significantly speed up the dynamics simulation of large molecular systems is presented herein. A multigranular modeling approach, whereby different parts of the molecule are modeled at different levels of detail, is enabled by substructuring. Substructuring the molecular system is accomplished by collecting groups of atoms into rigid or flexible bodies. Body flexibility is modeled by a truncated set of body-based modes. This approach allows for the elimination of the high-frequency harmonic motion while capturing the low-frequency anharmonic motion of interest. This results in the use of larger integration step sizes, substantially reducing the computational time required for a given dynamic simulation. The method also includes the use of a multiple time scale (MTS) integration scheme. Speed increases of 5- to 30-fold over atomistic simulations have been realized in various applications of the method. (C) 2000 John Wiley \& Sons, Inc.},
915 Author = {Chun, HM and Padilla, CE and Chin, DN and Watanabe, M and Karlov, VI and Alper, HE and Soosaar, K and Blair, KB and Becker, OM and Caves, LSD and Nagle, R and Haney, DN and Farmer, BL},
916 Date-Added = {2008-01-22 10:38:33 -0500},
917 Date-Modified = {2008-01-22 10:38:49 -0500},
918 Journal = jcc,
919 Keywords = {molecular dynamics; normal modes; anharmonicity; macromolecules; numerical integrators},
920 Pages = {159--184},
921 Timescited = 0,
922 Title = {{MBO(N)D:} A multibody method for long-time molecular dynamics simulations},
923 Volume = 21,
924 Year = 2000}
925
926 @article{Fogolari:1996lr,
927 Abstract = {In an effort to reduce the number of degrees of freedom necessary to describe a polypeptide chain we analyze the statistical behavior of polypeptide chains when represented as C alpha chains, C alpha chains with C beta atoms attached, and C alpha chains with rotational ellipsoids as models of side chains. A statistical analysis on a restricted data set of 75 unrelated protein structures is performed. The comparison of the database distributions with those obtained by model calculation on very short polypeptide stretches allows the dissection of local versus nonlocal features of the distributions. The database distribution of the bend angles of polypeptide chains of pseudo bonded C alpha atoms spans a restricted range of values and shows a bimodal structure. On the other hand, the torsion angles of the C alpha chain may assume almost all possible values. The distribution is bimodal, but with a much broader probability distribution than for bend angles. The C alpha - C beta vectors may be taken as representative of the orientation of the lateral chain, as the direction of the bond is close to the direction of the vector joining C alpha to the ad hoc defined center of the "steric mass" of the side chain. Interestingly, both the bend angle defined by C alpha i-C alpha i+1-C beta i+1 and the torsional angle offset of the pseudo-dihedral C alpha i-C alpha i+1-C alpha i+2-C beta i+2 with respect to C alpha i-C alpha i+1-C alpha i+2-C alpha i+3 span a limited range of values. The latter results show that it is possible to give a more realistic representation of polypeptide chains without introducing additional degrees of freedom, i.e., by just adding to the C alpha chain a C beta with given side-chain properties. However, a more realistic description of side chains may be attained by modeling side chains as rotational ellipsoids that have roughly the same orientation and steric hindrance. To this end, we define the steric mass of an atom as proportional to its van der Waals volume and we calculate the side-chain inertia ellipsoid assuming that the steric mass of each atom is uniformly distributed within its van der Waals volume. Finally, we define the rotational ellipsoid representing the side chain as the uniform density ellipsoid possessing the same rotationally averaged inertia tensor of the side chain. The statistics of ellipsoid parameters support the possibility of representing a side chain via an ellipsoid, independently of the local conformation. To make this description useful for molecular modeling we describe ellipsoid-ellipsoid interactions via a Lennard-Jones potential that preserves the repulsive core of the interacting ellipsoids and takes into account their mutual orientation. Tests are performed for two different forms of the interaction potential on a set of high-resolution protein structures. Results are encouraging, in view of the drastic simplifications that were introduced.},
928 Address = {Dipartimento di Scienze e Tecnologie Biomediche, Universita di Udine, Italy.},
929 Au = {Fogolari, F and Esposito, G and Viglino, P and Cattarinussi, S},
930 Author = {Fogolari, F and Esposito, G and Viglino, P and Cattarinussi, S},
931 Da = {19960924},
932 Date-Added = {2008-01-22 10:19:04 -0500},
933 Date-Modified = {2008-01-22 10:19:09 -0500},
934 Dcom = {19960924},
935 Edat = {1996/03/01},
936 Issn = {0006-3495 (Print)},
937 Jid = {0370626},
938 Journal = {Biophys J},
939 Jt = {Biophysical journal},
940 Language = {eng},
941 Lr = {20071115},
942 Mh = {Amino Acids/chemistry; Biophysics; Carbon/chemistry; Databases, Factual; Evaluation Studies as Topic; *Models, Molecular; Molecular Structure; Peptides/*chemistry; *Protein Conformation; Software; Thermodynamics},
943 Mhda = {1996/03/01 00:01},
944 Number = {3},
945 Own = {NLM},
946 Pages = {1183--1197},
947 Pl = {UNITED STATES},
948 Pmid = {8785277},
949 Pst = {ppublish},
950 Pt = {Journal Article},
951 Pubm = {Print},
952 Rn = {0 (Amino Acids); 0 (Peptides); 7440-44-0 (Carbon)},
953 Sb = {IM},
954 So = {Biophys J. 1996 Mar;70(3):1183-97.},
955 Stat = {MEDLINE},
956 Title = {Modeling of polypeptide chains as C alpha chains, C alpha chains with C beta, and C alpha chains with ellipsoidal lateral chains.},
957 Volume = {70},
958 Year = {1996}}
959
960 @inbook{Ramachandran1996,
961 Address = {Providence, Rhode Island},
962 Author = {Gomathi Ramachandran and Tamar Schlick},
963 Chapter = {Beyond optimization: Simulating the dynamics of supercoiled DNA by a macroscopic model},
964 Date-Added = {2008-01-22 10:03:42 -0500},
965 Date-Modified = {2008-01-22 10:06:57 -0500},
966 Editor = {P. M. Pardalos and D. Shalloway and G. Xue},
967 Pages = {215-231},
968 Publisher = {American Mathematical Society},
969 Series = {DIMACS Series in Discrete Mathematics and Theoretical Computer Science},
970 Title = {Global Minimization of Nonconvex Energy Functions: Molecular Conformation and Protein Folding},
971 Volume = {23},
972 Year = {1996}}
973
974 @article{FIXMAN:1986lr,
975 Author = {Fixman, M},
976 Date-Added = {2008-01-22 09:59:29 -0500},
977 Date-Modified = {2008-01-22 09:59:35 -0500},
978 Journal = {Macromolecules},
979 Pages = {1204-1207},
980 Timescited = {0},
981 Title = {CONSTRUCTION OF LANGEVIN FORCES IN THE SIMULATION OF HYDRODYNAMIC INTERACTION},
982 Volume = {19},
983 Year = {1986}}
984
985 @article{Berendsen87,
986 Author = {H.~J.~C. Berendsen and J.~R. Grigera and T.~P. Straatsma},
987 Date-Added = {2008-01-22 09:53:15 -0500},
988 Date-Modified = {2008-01-22 09:53:15 -0500},
989 Journal = jpc,
990 Pages = {6269-6271},
991 Title = {The Missing Term in Effective Pair Potentials},
992 Volume = 91,
993 Year = 1987}
994
995 @incollection{Berendsen81,
996 Address = {Dordrecht},
997 Author = {H.~J.~C. Berendsen and J.~P.~M. Postma and W.~F. {van~Gunsteren} and J. Hermans},
998 Booktitle = {Intermolecular Forces},
999 Date-Added = {2008-01-22 09:52:49 -0500},
1000 Date-Modified = {2008-01-22 09:52:49 -0500},
1001 Editor = {B. Pullman},
1002 Pages = {331-342},
1003 Publisher = {Reidel},
1004 Title = {Simple Point Charge Water},
1005 Year = 1981}
1006
1007 @article{Stillinger74,
1008 Author = {F.~H. Stillinger and A. Rahman},
1009 Date-Added = {2008-01-22 09:51:43 -0500},
1010 Date-Modified = {2008-01-22 09:51:43 -0500},
1011 Journal = jcp,
1012 Number = 4,
1013 Pages = {1545-1557},
1014 Title = {Improved simulation of liquid water by molecular dynamics},
1015 Volume = 60,
1016 Year = 1974}
1017
1018 @article{Torre:1983lr,
1019 Author = {{Garc\'{i}a de la Torre}, Jose and Rodes, Vicente},
1020 Date-Added = {2008-01-11 16:16:43 -0500},
1021 Date-Modified = {2008-01-11 16:16:43 -0500},
1022 Journal = jcp,
1023 Journal1 = {The Journal of Chemical Physics},
1024 Journal2 = {J. Chem. Phys.},
1025 Keywords = {polymers; molecular models; hydrodynamics; rotation; interactions; macromolecules},
1026 Number = 5,
1027 Pages = {2454--2460},
1028 Publisher = {AIP},
1029 Title = {Effects from bead size and hydrodynamic interactions on the translational and rotational coefficients of macromolecular bead models},
1030 Ty = {JOUR},
1031 Url = {http://link.aip.org/link/?JCP/79/2454/1},
1032 Volume = 79,
1033 Year = 1983,
1034 Bdsk-Url-1 = {http://link.aip.org/link/?JCP/79/2454/1}}
1035
1036 @article{PhysRev.119.53,
1037 Author = {Favro, L. Dale},
1038 Date-Added = {2008-01-09 16:57:02 -0500},
1039 Date-Modified = {2008-01-09 16:57:02 -0500},
1040 Doi = {10.1103/PhysRev.119.53},
1041 Journal = {Phys. Rev.},
1042 Month = {Jul},
1043 Number = 1,
1044 Numpages = 9,
1045 Pages = {53--62},
1046 Publisher = {American Physical Society},
1047 Title = {Theory of the Rotational Brownian Motion of a Free Rigid Body},
1048 Volume = 119,
1049 Year = 1960,
1050 Bdsk-Url-1 = {http://dx.doi.org/10.1103/PhysRev.119.53}}
1051
1052 @article{hess:209,
1053 Author = {Berk Hess},
1054 Date-Added = {2008-01-08 16:41:06 -0500},
1055 Date-Modified = {2008-01-08 16:41:06 -0500},
1056 Doi = {10.1063/1.1421362},
1057 Journal = jcp,
1058 Keywords = {viscosity; molecular dynamics method; liquid theory; shear flow},
1059 Number = 1,
1060 Pages = {209-217},
1061 Publisher = {AIP},
1062 Title = {Determining the shear viscosity of model liquids from molecular dynamics simulations},
1063 Url = {http://link.aip.org/link/?JCP/116/209/1},
1064 Volume = 116,
1065 Year = 2002,
1066 Bdsk-Url-1 = {http://link.aip.org/link/?JCP/116/209/1},
1067 Bdsk-Url-2 = {http://dx.doi.org/10.1063/1.1421362}}
1068
1069 @article{Garcia-de-la-Torre:1997qy,
1070 Abstract = {Single-valued hydrodynamic coefficients of a rigid particle can be calculated from existing theories and computer programs for either bead models or ellipsoids. Starting from these coefficients, we review the procedures for the calculation of complex solution properties depending on rotational diffusion, such as the decays of electric birefringence and fluorescence anisotropy. We also describe the calculation of the scattering from factor of bead models. The hydrodynamic coefficients and solution properties can be combined to give universal, shape-dependent functions, which were initially intended for ellipsoidal particles, and are extended here for the most general case. We have implemented all three developments in a new computer program. SOLPRO, for calculation of SOLution PROperties, which can be linked to existing software for bead models or ellipsoids.},
1071 Address = {Departamento de Quimica Fisica Universidad de Murcia, Spain. jgt{\char64}fcu,um.es},
1072 Au = {{Garc\'{i}a de la Torre}, Jose and Carrasco, B and Harding, SE},
1073 Author = {{Garc\'{i}a de la Torre}, Jose and Carrasco, B and Harding, S E},
1074 Da = 19970709,
1075 Date-Added = {2008-01-08 15:45:31 -0500},
1076 Date-Modified = {2008-01-08 15:46:57 -0500},
1077 Dcom = 19970709,
1078 Edat = {1997/01/01},
1079 Issn = {0175-7571 (Print)},
1080 Jid = 8409413,
1081 Journal = {Eur Biophys J},
1082 Jt = {European biophysics journal : EBJ},
1083 Keywords = {Birefringence; Fluorescence Polarization; Humans; Immunoglobulin G/chemistry; Models, Structural; *Protein Conformation; Proteins/*chemistry; Scattering, Radiation; *Software; Ultracentrifugation/methods},
1084 Language = {eng},
1085 Lr = 20061115,
1086 Mhda = {1997/01/01 00:01},
1087 Number = {5-6},
1088 Own = {NLM},
1089 Pages = {361--372},
1090 Pl = {GERMANY},
1091 Pmid = 9213556,
1092 Pst = {ppublish},
1093 Pt = {Journal Article; Research Support, Non-U.S. Gov't},
1094 Pubm = {Print},
1095 Rn = {0 (Immunoglobulin G); 0 (Proteins)},
1096 Sb = {IM},
1097 So = {Eur Biophys J. 1997;25(5-6):361-72.},
1098 Stat = {MEDLINE},
1099 Title = {SOLPRO: theory and computer program for the prediction of SOLution PROperties of rigid macromolecules and bioparticles.},
1100 Volume = 25,
1101 Year = 1997}
1102
1103 @article{Ravichandran:1999fk,
1104 Abstract = {Detailed molecular dynamics simulations of the rotational and the translational motions of Gay-Berne ellipsoids in a sea of Lennard-Jones spheres have been carried out. It is found that while the translational motion of an ellipsoid is isotropic at low density, it becomes increasingly anisotropic with density until the ratio of the parallel to the perpendicular diffusion coefficients becomes nearly equal to the value of the aspect ratio at high density. The latter is in agreement with the prediction of Navier-Stokes hydrodynamics with slip boundary condition. The product of the translational diffusion coefficient and the rotational correlation time also attains a hydrodynamic-like density independent behavior only at high density. The reorientational correlation function becomes nonexponential at high density and low temperature where it also develops a slow decay. The perpendicular component of the velocity time correlation function exhibits a clear double minimum, only at high density, which becomes more pronounced as the aspect ratio is increased. (C) 1999 American Institute of Physics. [S0021-9606(99)51440-2].},
1105 Author = {Ravichandran, S and Bagchi, B},
1106 Date-Added = {2008-01-08 15:24:48 -0500},
1107 Date-Modified = {2008-01-08 15:25:41 -0500},
1108 Journal = jcp,
1109 Pages = {7505-7511},
1110 Title = {Anisotropic diffusion of nonspherical molecules in dense liquids: A molecular dynamics simulation of isolated ellipsoids in the sea of spheres},
1111 Volume = 111,
1112 Year = 1999}
1113
1114 @article{TANG:1993lr,
1115 Abstract = {Translational friction coefficients of hard prolate ellipsoids (having aspect ratios of 1-10) have been calculated by solving the linearized Navier-Stokes equations of hydrodynamics, using the method of Faxen's theorem. When the stick boundary condition was used, the present results reproduce the famous work of Lamb. The new information derived from this study arises from the analysis of the friction under the influence of the slip hydrodynamic boundary condition. It was found that the slip friction perpendicular to the long axis of the prolate ellipsoid increases monotonically with aspect ratio, whereas the parallel component of the friction decreases monotonically to an apparent limiting value. The ratio f(perpendicular to)/f(parallel to) of friction coefficients perpendicular and parallel to the long axis of the particle, calculated using slip hydrodynamics, scales roughly as the aspect ratio of the ellipsoid, in accord with the findings from an Enskog (uncorrelated binary collision) kinetic theory of hard ellipsoids and from the estimate derived from molecular dynamics. In contrast, f(perpendicular to)/f(parallel to) derived by means of stick hydrodynamics shows a weak dependence on the aspect ratio and disagrees with kinetic theory and molecular dynamics findings.},
1116 Author = {TANG, SA and EVANS, GT},
1117 Date-Added = {2008-01-08 15:23:42 -0500},
1118 Date-Modified = {2008-01-08 15:24:09 -0500},
1119 Journal = mp,
1120 Pages = {1443-1457},
1121 Title = {A CRITIQUE OF SLIP AND STICK HYDRODYNAMICS FOR ELLIPSOIDAL BODIES},
1122 Volume = 80,
1123 Year = 1993}
1124
1125 @article{Schmidt:2003kx,
1126 Abstract = {Using molecular dynamics computer simulation, we have calculated the velocity autocorrelation function and diffusion constant for a spherical solute in a dense fluid of spherical solvent particles. The size and mass of the solute particle are related in such a way that we can naturally approach the Brownian limit (when the solute becomes much larger and more massive than the solvent particles). We find that as long as the solute radius is interpreted as an effective hydrodynamic radius, the Stokes-Einstein law with slip boundary conditions is satisfied as the Brownian limit is approached (specifically, when the solute is roughly 100 times more massive than the solvent particles). In contrast, the Stokes-Einstein law is not satisfied for a tagged particle of the neat solvent. We also find that in the Brownian limit the amplitude of the long-time tail of the solute's velocity autocorrelation function is in good agreement with theoretical hydrodynamic predictions. When the solvent density is substantially lower than the triple density, the Stokes-Einstein law is no longer satisfied, and the amplitude of the long-time tail is not in good agreement with theoretical predictions, signaling the breakdown of hydrodynamics. (C) 2003 American Institute of Physics.},
1127 Author = {Schmidt, JR and Skinner, JL},
1128 Date-Added = {2008-01-08 15:12:53 -0500},
1129 Date-Modified = {2008-01-08 15:13:21 -0500},
1130 Doi = {DOI 10.1063/1.1610442},
1131 Journal = jcp,
1132 Pages = {8062-8068},
1133 Title = {Hydrodynamic boundary conditions, the Stokes-Einstein law, and long-time tails in the Brownian limit},
1134 Volume = 119,
1135 Year = 2003,
1136 Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.1610442}}
1137
1138 @article{Schmidt:2004fj,
1139 Abstract = {Using molecular dynamics computer simulation, we have calculated the velocity autocorrelation function and diffusion constant for a variety of solutes in a dense fluid of spherical solvent particles. We explore the effects of surface roughness of the solute on the resulting hydrodynamic boundary condition as we naturally approach the Brownian limit (when the solute becomes much larger and more massive than the solvent particles). We find that when the solute and solvent interact through a purely repulsive isotropic potential, in the Brownian limit the Stokes-Einstein law is satisfied with slip boundary conditions. However, when surface roughness is introduced through an anisotropic solute-solvent interaction potential, we find that the Stokes-Einstein law is satisfied with stick boundary conditions. In addition, when the attractive strength of a short-range isotropic solute-solvent potential is increased, the solute becomes dressed with solvent particles, making it effectively rough, and so stick boundary conditions are again recovered.},
1140 Author = {Schmidt, JR and Skinner, JL},
1141 Date-Added = {2008-01-08 15:12:53 -0500},
1142 Date-Modified = {2008-01-08 15:13:20 -0500},
1143 Doi = {DOI 10.1021/jp037185r},
1144 Journal = jpcb,
1145 Pages = {6767-6771},
1146 Title = {Brownian motion of a rough sphere and the Stokes-Einstein Law},
1147 Volume = 108,
1148 Year = 2004,
1149 Bdsk-Url-1 = {http://dx.doi.org/10.1021/jp037185r}}
1150
1151 @article{Klein01,
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1153 Date-Added = {2008-01-08 14:58:56 -0500},
1154 Date-Modified = {2008-01-08 14:58:56 -0500},
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1163 Date-Added = {2008-01-08 14:58:56 -0500},
1164 Date-Modified = {2008-01-08 14:58:56 -0500},
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1169 Year = 1998}
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1297 Date-Added = {2008-01-08 14:58:56 -0500},
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1350 Journal = {J. Chem. Phys.},
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1465 Date-Modified = {2008-01-08 14:58:57 -0500},
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1579 Date-Added = {2008-01-08 14:58:56 -0500},
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1600 Date-Modified = {2008-01-08 14:58:57 -0500},
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1618 @article{NorbertKucerka06012006,
1619 Abstract = {X-ray data are presented for the benchmark dipalmitoylphosphatidylcholine lipid bilayer in the most biologically relevant state in which the bilayers are fully hydrated and in the fluid (liquid-crystalline) phase. Form factors F(qz) are obtained from a combination of two sample preparations, oriented stacks of bilayers for qz extending to 0.85 A-1 and unilamellar vesicles for smaller qz. Modeling obtains the electron density profile and values for the area per molecule, for the locations of the component groups, and for the different types of thicknesses of the bilayer, such as the hydrocarbon thickness and the steric thickness.
1620 },
1621 Author = {Kucerka, Norbert and Tristram-Nagle, Stephanie and Nagle, John F.},
1622 Date-Added = {2008-01-08 14:58:56 -0500},
1623 Date-Modified = {2008-01-08 14:58:57 -0500},
1624 Doi = {10.1529/biophysj.106.086017},
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1627 Number = 11,
1628 Pages = {L83-85},
1629 Title = {{Closer Look at Structure of Fully Hydrated Fluid Phase DPPC Bilayers}},
1630 Url = {http://www.biophysj.org/cgi/content/abstract/90/11/L83},
1631 Volume = 90,
1632 Year = 2006,
1633 Bdsk-Url-1 = {http://www.biophysj.org/cgi/content/abstract/90/11/L83},
1634 Bdsk-Url-2 = {http://dx.doi.org/10.1529/biophysj.106.086017}}
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1935 Author = {F.~H. Stillinger and T.~A. Weber},
1936 Date-Added = {2008-01-08 14:58:56 -0500},
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1945 @article{Hunenberger99b,
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1948 Date-Modified = {2008-01-08 14:58:58 -0500},
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1951 Pages = {69-88},
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1956 @article{Spohr97,
1957 Author = {E. Spohr},
1958 Date-Added = {2008-01-08 14:58:56 -0500},
1959 Date-Modified = {2008-01-08 14:58:58 -0500},
1960 Journal = {J. Chem. Phys.},
1961 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Ewald/Spohr_2DElectrostatics_97.pdf},
1962 Number = 16,
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1968 @article{Marrink01b,
1969 Author = {S.~J. Marrink and A.~E. Mark},
1970 Date-Added = {2008-01-08 14:58:56 -0500},
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1979 Author = {K.~C. Tu and M. Tarek and M.~L. Klein and D. Scharf},
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2111 Title = {Electrostatics in periodic slab geometries. I},
2112 Volume = 117,
2113 Year = 2002,
2114 Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.149195}}
2115
2116 @article{deJoannis02,
2117 Author = {J. {de Joannis} and A. Arnold and C. Holm},
2118 Date-Added = {2008-01-08 14:58:56 -0500},
2119 Date-Modified = {2008-01-08 14:58:58 -0500},
2120 Doi = {10.1063/1.149195},
2121 Journal = {J. Chem. Phys.},
2122 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Ewald/Joannis_SlabElectrostatics_02.pdf},
2123 Number = 6,
2124 Pages = {2503-2512},
2125 Title = {Electrostatics in periodic slab geometries. II},
2126 Volume = 117,
2127 Year = 2002,
2128 Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.149195}}
2129
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2133 Date-Modified = {2008-01-08 14:58:58 -0500},
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2138 Year = 1995}
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2142 Date-Added = {2008-01-08 14:58:56 -0500},
2143 Date-Modified = {2008-01-08 14:58:58 -0500},
2144 Journal = pre,
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2148 Year = 1996}
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2163 Date-Added = {2008-01-08 14:58:56 -0500},
2164 Date-Modified = {2008-01-08 14:58:58 -0500},
2165 Journal = prb,
2166 Number = 12,
2167 Pages = 7983,
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2170 Year = 1986}
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2175 Date-Modified = {2008-01-08 14:58:58 -0500},
2176 Journal = {J. Phys. Chem. B},
2177 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/WolfApplications/Zahn_enhancedWolfH2O_02.pdf},
2178 Number = 41,
2179 Pages = {10725-10732},
2180 Title = {Enhancement of the Wolf Damped Coulomb Potential: Static, Dynamic, and Dielectric Properties of Liquid Water from Molecular Simulation},
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2182 Year = 2002}
2183
2184 @article{Metropolis53,
2185 Author = {N. Metropolis and A.~W. Rosenbluth and M.~N. Rosenbluth and A.~H. Teller and E. Teller},
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2187 Date-Modified = {2008-01-08 14:58:58 -0500},
2188 Journal = {J. Chem. Phys.},
2189 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Metropolis_MCCalculations_53.pdf},
2190 Pages = {1087-1092},
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2192 Volume = 21,
2193 Year = 1953}
2194
2195 @article{Parry76,
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2215 @article{Todorova2004,
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2217 Date-Added = {2008-01-08 14:58:56 -0500},
2218 Date-Modified = {2008-01-08 14:58:59 -0500},
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2222 Volume = 14,
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2225 @article{Hunenberger99a,
2226 Author = {P.~H. H\"{u}nenberger and J.~A. McCammon},
2227 Date-Added = {2008-01-08 14:58:56 -0500},
2228 Date-Modified = {2008-01-08 14:58:59 -0500},
2229 Journal = {J. Chem. Phys.},
2230 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Ewald/Hunenberger_IonSolutionEwaldArtifacts_99.pdf},
2231 Number = 4,
2232 Pages = {1856-1872},
2233 Title = {Ewald artifacts in computer simulations of ionic solvation and ion -- ion interaction: A continuum electrostatics study},
2234 Volume = 110,
2235 Year = 1999}
2236
2237 @article{Rhee89,
2238 Author = {Y.-J. Rhee and J.~W. Halley and J. Hautman and A. Rahman},
2239 Date-Added = {2008-01-08 14:58:56 -0500},
2240 Date-Modified = {2008-01-08 14:58:59 -0500},
2241 Journal = {Phys. Rev. B},
2242 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Ewald/Rhee_finiteDimensionEwald_88.pdf},
2243 Number = 1,
2244 Pages = {36-42},
2245 Title = {Ewald methods in molecular dynamics for systems of finite extent in one of three dimensions},
2246 Volume = 40,
2247 Year = 1989}
2248
2249 @article{Yeh99,
2250 Author = {I.-C. Yeh and M.~L. Berkowitz},
2251 Date-Added = {2008-01-08 14:58:56 -0500},
2252 Date-Modified = {2008-01-08 14:58:59 -0500},
2253 Journal = {J. Chem. Phys.},
2254 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Ewald/Yeh_SlabCorrectionEwald_99.pdf},
2255 Number = 7,
2256 Pages = {3155-3162},
2257 Title = {Ewald summation for systems with slab geometry},
2258 Volume = 111,
2259 Year = 1999}
2260
2261 @article{Brodka04,
2262 Author = {A. Br\'{o}dka},
2263 Date-Added = {2008-01-08 14:58:56 -0500},
2264 Date-Modified = {2008-01-08 14:58:59 -0500},
2265 Doi = {10.1016/j.cplett.2004.10.086},
2266 Journal = {Chem. Phys. Lett.},
2267 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Ewald/Brodka_PointDipoleSlabEwald_04.pdf},
2268 Pages = {62-67},
2269 Title = {Ewald summation method with electrostatic layer correction for interactions of point dipoles in slab geometry},
2270 Volume = 400,
2271 Year = 2004,
2272 Bdsk-Url-1 = {http://dx.doi.org/10.1016/j.cplett.2004.10.086}}
2273
2274 @article{Chuang98,
2275 Author = {I. Chuang and N. Gershenfeld and M. Kubinec},
2276 Date-Added = {2008-01-08 14:58:56 -0500},
2277 Date-Modified = {2008-01-08 14:58:59 -0500},
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2282 Year = 1998}
2283
2284 @article{Banerjee02,
2285 Author = {Srilekha Banerjee},
2286 Date-Added = {2008-01-08 14:58:56 -0500},
2287 Date-Modified = {2008-01-08 14:58:59 -0500},
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2294 @article{Bannerjee02,
2295 Author = {S. Bannerjee},
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2297 Date-Modified = {2008-01-08 14:58:59 -0500},
2298 Journal = {Physica A},
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2302 Year = 2002}
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2304 @article{Cleaver96,
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2306 Date-Added = {2008-01-08 14:58:56 -0500},
2307 Date-Modified = {2008-01-08 14:58:59 -0500},
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2336 @article{Benninger:2005qy,
2337 Abstract = {The plasma membrane of cells is an ordered environment, giving rise to anisotropic orientation and restricted motion of molecules and proteins residing in the membrane. At the same time as being an organized matrix of defined structure, the cell membrane is heterogeneous and dynamic. Here we present a method where we use fluorescence imaging of linear dichroism to measure the orientation of molecules relative to the cell membrane. By detecting linear dichroism as well as fluorescence anisotropy, the orientation parameters are separated from dynamic properties such as rotational diffusion and homo energy transfer (energy migration). The sensitivity of the technique is enhanced by using two-photon excitation for higher photo-selection compared to single photon excitation. We show here that we can accurately image lipid organization in whole cell membranes and in delicate structures such as membrane nanotubes connecting two cells. The speed of our wide-field imaging system makes it possible to image changes in orientation and anisotropy occurring on a subsecond timescale. This is demonstrated by time-lapse studies showing that cholesterol depletion rapidly disrupts the orientation of a fluorophore located within the hydrophobic region of the cell membrane but not of a surface bound probe. This is consistent with cholesterol having an important role in stabilizing and ordering the lipid tails within the plasma membrane. },
2338 Annote = {10.1529/biophysj.104.050096},
2339 Author = {Benninger, Richard K. P. and Onfelt, Bjorn and Neil, Mark A. A. and Davis, Daniel M. and French, Paul M. W.},
2340 Date-Added = {2008-01-08 14:58:56 -0500},
2341 Date-Modified = {2008-01-08 14:58:59 -0500},
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2344 Number = 1,
2345 Pages = {609--622},
2346 Title = {Fluorescence Imaging of Two-Photon Linear Dichroism: Cholesterol Depletion Disrupts Molecular Orientation in Cell Membranes},
2347 Ty = {JOUR},
2348 Url = {http://www.biophysj.org/cgi/content/abstract/88/1/609},
2349 Volume = 88,
2350 Year = 2005,
2351 Bdsk-Url-1 = {http://www.biophysj.org/cgi/content/abstract/88/1/609}}
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2353 @inbook{Blumen86,
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2356 Chapter = {Reactions in Disordered Media Modelled by Fractals},
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2358 Date-Modified = {2008-01-08 14:58:59 -0500},
2359 Editor = {Luciano Peitronero and E. Tosatti},
2360 Pages = 399,
2361 Publisher = {North-Holland},
2362 Series = {International Symposium on Fractals in Physics},
2363 Title = {Fractals in Physics},
2364 Year = 1986}
2365
2366 @article{Marland1979,
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2368 Date-Added = {2008-01-08 14:58:56 -0500},
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2372 Pages = {1618-1621},
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2374 Volume = 43,
2375 Year = 1979}
2376
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2385 Year = 1972}
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2387 @article{Golubkov06,
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2534 Publisher = {Oxford University Press},
2535 Title = {Introduction to Modern Statistical Mechanics},
2536 Year = 1987}
2537
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2540 Date-Added = {2008-01-08 14:58:56 -0500},
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2545 Volume = 218,
2546 Year = 1994}
2547
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2552 Journal = {J. Chem. Phys.},
2553 Local-Url = {file://localhost/Users/cfennell/Documents/pdf_files/TheoryTechniques/Ewald/Luty_LatticeSumElectrostatics_95.pdf},
2554 Number = 8,
2555 Pages = {3014-3021},
2556 Title = {Lattice-sum methods for calculating electrostatic interactions in molecular simulations},
2557 Volume = 103,
2558 Year = 1995}
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2562 Date-Added = {2008-01-08 14:58:56 -0500},
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2567 Volume = 100,
2568 Year = 1994}
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2570 @article{Sutton90,
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2581 Author = {D. Bassolino and H.~E. Alper and T.~R. Stouch},
2582 Date-Added = {2008-01-08 14:58:56 -0500},
2583 Date-Modified = {2008-01-08 14:58:59 -0500},
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2585 Pages = {4118-4129},
2586 Title = {MECHANISM OF SOLUTE DIFFUSION THROUGH LIPID BILAYER-MEMBRANES BY MOLECULAR-DYNAMICS SIMULATION},
2587 Volume = 117,
2588 Year = 1995}
2589
2590 @article{Lindahl00,
2591 Author = {E. Lindahl and O. Edholm},
2592 Date-Added = {2008-01-08 14:58:56 -0500},
2593 Date-Modified = {2008-01-08 14:58:59 -0500},
2594 Journal = bj,
2595 Month = {July},
2596 Pages = {426-433},
2597 Title = {Mesoscopic undulations and thickness fluctuations in lipid bilayers from molecular dynamics simulations},
2598 Volume = 79,
2599 Year = 2000}
2600
2601 @article{Gezelter99,
2602 Author = {J.~D. Gezelter and E. Rabani and B.~J. Berne},
2603 Date-Added = {2008-01-08 14:58:56 -0500},
2604 Date-Modified = {2008-01-08 14:58:59 -0500},
2605 Journal = jcp,
2606 Pages = 3444,
2607 Title = {Methods for calculating the hopping rate for orientational and spatial diffusion in a molecular liquid: $\mbox{CS}_{2}$},
2608 Volume = 110,
2609 Year = 1999}
2610
2611 @article{Sun97b,
2612 Author = {X. Sun and W.~H. Miller},
2613 Date-Added = {2008-01-08 14:58:56 -0500},
2614 Date-Modified = {2008-01-08 14:58:59 -0500},
2615 Journal = jcp,
2616 Pages = 916,
2617 Title = {Mixed semiclassical-classical approaches to the dynamics of complex molecular systems},
2618 Year = 1997}
2619
2620 @article{Goldstein88,
2621 Author = {Raymond E. Goldstein and Stanislas Leibler},
2622 Date-Added = {2008-01-08 14:58:56 -0500},
2623 Date-Modified = {2008-01-08 14:58:59 -0500},
2624 Journal = prl,
2625 Number = 19,
2626 Pages = {2213-2216},
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3600 @article{NorbertKucerka04012005,
3601 Abstract = {Quantitative structures of the fully hydrated fluid phases of dimyristoylphosphatidylcholine (DMPC) and dilauroylphosphatidylcholine (DLPC) were obtained at 30{degrees}C. Data for the relative form factors F(qz) for DMPC were obtained using a combination of four methods. 1), Volumetric data provided F(0). 2), Diffuse x-ray scattering from oriented stacks of bilayers provided relative form factors |F(qz)| for high qz, 0.22 < qz < 0.8 A-1. 3), X-ray scattering from extruded unilamellar vesicles with diameter 600 A provided |F(qz)| for low qz, 0.1 < qz < 0.3 A-1. 4), Previous measurements using a liquid crystallographic x-ray method provided |F(2{pi}h/D)| for h = 1 and 2 for a range of nearly fully hydrated D-spacings. The data from method 4 overlap and validate the new unilamellar vesicles data for DMPC, so method 4 is not required for DLPC or future studies. We used hybrid electron density models to obtain structural results from these form factors. Comparison of the model electron density profiles with that of gel phase DMPC provides areas per lipid A, 60.6 {+/-} 0.5 A2 for DMPC and 63.2 {+/-} 0.5 A2 for DLPC. Constraints on the model provided by volume measurements and component volumes obtained from simulations put the electron density profiles {rho}(z) and the corresponding form factors F(qz) on absolute scales. Various thicknesses, such as the hydrophobic thickness and the steric thickness, are obtained and compared to literature values.
3602 },
3603 Author = {Kucerka, Norbert and Liu, Yufeng and Chu, Nanjun and Petrache, Horia I. and Tristram-Nagle, Stephanie and Nagle, John F.},
3604 Date-Added = {2008-01-08 14:58:56 -0500},
3605 Date-Modified = {2008-01-08 14:59:02 -0500},
3606 Doi = {10.1529/biophysj.104.056606},
3607 Eprint = {http://www.biophysj.org/cgi/reprint/88/4/2626.pdf},
3608 Journal = {Biophys. J.},
3609 Number = 4,
3610 Pages = {2626-2637},
3611 Title = {{Structure of Fully Hydrated Fluid Phase DMPC and DLPC Lipid Bilayers Using X-Ray Scattering from Oriented Multilamellar Arrays and from Unilamellar Vesicles}},
3612 Url = {http://www.biophysj.org/cgi/content/abstract/88/4/2626},
3613 Volume = 88,
3614 Year = 2005,
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3617
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3619 Author = {Olaf Lenz and Friederike Schmid},
3620 Date-Added = {2008-01-08 14:58:56 -0500},
3621 Date-Modified = {2008-01-08 14:59:02 -0500},
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3631 Date-Added = {2008-01-08 14:58:56 -0500},
3632 Date-Modified = {2008-01-08 14:59:02 -0500},
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3636 Volume = 93,
3637 Year = 1996}
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3641 Date-Added = {2008-01-08 14:58:56 -0500},
3642 Date-Modified = {2008-01-08 14:59:02 -0500},
3643 Journal = pre,
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3647 Volume = 68,
3648 Year = 2003}
3649
3650 @article{Liu92,
3651 Author = {R.~S. Liu and D.~W. Qi and S. Wang},
3652 Date-Added = {2008-01-08 14:58:56 -0500},
3653 Date-Modified = {2008-01-08 14:59:02 -0500},
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3658 Year = 1992}
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3663 Date-Modified = {2008-01-08 14:59:02 -0500},
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3668 Year = 1996}
3669
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3677 Volume = 254,
3678 Year = 1979}
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3682 Date-Added = {2008-01-08 14:58:56 -0500},
3683 Date-Modified = {2008-01-08 14:59:02 -0500},
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3699 Year = 2000}
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3702 Author = {W. Kob and H.~C. Andersen},
3703 Date-Added = {2008-01-08 14:58:56 -0500},
3704 Date-Modified = {2008-01-08 14:59:02 -0500},
3705 Journal = pre,
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3708 Volume = 51,
3709 Year = 1995}
3710
3711 @article{Kob95b,
3712 Author = {W. Kob and H.~C. Andersen},
3713 Date-Added = {2008-01-08 14:58:56 -0500},
3714 Date-Modified = {2008-01-08 14:59:02 -0500},
3715 Journal = pre,
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3719 Year = 1995}
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3730 Year = 1979}
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3740 Year = 1992}
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3823 Year = 1983}
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3919 Year = 1986}
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3926 Pages = {6559-6561},
3927 Title = {Theory of the intermediate rippled phase of phospholipid bilayers},
3928 Volume = 81,
3929 Year = 1984}
3930
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3937 Title = {They're not Dumb. They're Different: Stalking the Second Tier},
3938 Year = 1990}
3939
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3948 Volume = 67,
3949 Year = 1991}
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3959 Volume = 102,
3960 Year = 1995}
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3970 Year = 1998}
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3974 Date-Added = {2008-01-08 14:58:56 -0500},
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3976 Journal = prl,
3977 Number = 20,
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3980 Volume = 80,
3981 Year = 1998}
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3986 Date-Modified = {2008-01-08 14:59:02 -0500},
3987 Journal = jcp,
3988 Pages = {5175-5176},
3989 Title = {Transport coefficients of liquid transition metals: A computer simulation study using the embedded atom model},
3990 Volume = 109,
3991 Year = 1998}
3992
3993 @article{Born12,
3994 Author = {M. Born and Th. Von~Karman},
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3997 Journal = {Physik Z.},
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4000 Volume = 13,
4001 Year = 1912}
4002
4003 @incollection{Angell85,
4004 Address = {Springfield, VA},
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4006 Booktitle = {Relaxations in Complex Systems},
4007 Date-Added = {2008-01-08 14:58:56 -0500},
4008 Date-Modified = {2008-01-08 14:59:03 -0500},
4009 Editor = {K.~Ngai and G.~B. Wright},
4010 Pages = 1,
4011 Publisher = {National Technical Information Service, U.S. Department of Commerce},
4012 Title = {unknown},
4013 Year = 1985}
4014
4015 @article{Ribeiro98,
4016 Author = {M.~C.~C. Ribeiro and P.~A. Madden},
4017 Date-Added = {2008-01-08 14:58:56 -0500},
4018 Date-Modified = {2008-01-08 14:59:03 -0500},
4019 Journal = jcp,
4020 Pages = {3256-3263},
4021 Title = {Unstable Modes in Ionic Melts},
4022 Volume = 108,
4023 Year = 1998}
4024
4025 @article{Mutz1991,
4026 Author = {Mutz, M. and Bensimon, D. and Brienne, M. J.},
4027 Date-Added = {2008-01-08 14:58:56 -0500},
4028 Date-Modified = {2008-01-08 14:59:03 -0500},
4029 Doi = {10.1103/PhysRevLett.67.923},
4030 Journal = {Phys. Rev. Lett.},
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4032 Number = 7,
4033 Numpages = 3,
4034 Pages = {923--926},
4035 Publisher = {American Physical Society},
4036 Title = {Wrinkling transition in partially polymerized vesicles},
4037 Volume = 67,
4038 Year = 1991,
4039 Bdsk-Url-1 = {http://dx.doi.org/10.1103/PhysRevLett.67.923}}
4040
4041 @article{Wendt78,
4042 Author = {H. Wendt and F.~F. Abraham},
4043 Date-Added = {2008-01-08 14:58:56 -0500},
4044 Date-Modified = {2008-01-08 14:59:03 -0500},
4045 Journal = prl,
4046 Pages = 1244,
4047 Volume = 41,
4048 Year = 1978}
4049
4050 @unpublished{Truhlar00,
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4052 Date-Added = {2008-01-08 14:58:56 -0500},
4053 Date-Modified = {2008-01-08 14:59:03 -0500},
4054 Note = {private correspondence},
4055 Year = 2000}
4056
4057 @article{Dwyer1977,
4058 Author = {D.~J. Dwyer and G.~W. Simmons and R.~P. Wei},
4059 Date-Added = {2008-01-08 14:58:56 -0500},
4060 Date-Modified = {2008-01-08 14:59:03 -0500},
4061 Journal = {Surf. Sci.},
4062 Pages = 617,
4063 Volume = 64,
4064 Year = 1977}
4065
4066 @article{Macritche78,
4067 Author = {F. MacRitche},
4068 Date-Added = {2008-01-08 14:58:56 -0500},
4069 Date-Modified = {2008-01-08 14:59:03 -0500},
4070 Journal = {Adv. Protein Chem.},
4071 Pages = 283,
4072 Volume = 32,
4073 Year = 1978}
4074
4075 @article{Feder80,
4076 Author = {J. Feder},
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4078 Date-Modified = {2008-01-08 14:59:03 -0500},
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4080 Pages = 237,
4081 Volume = 87,
4082 Year = 1980}
4083
4084 @article{Ramsden93,
4085 Author = {J.~J. Ramsden},
4086 Date-Added = {2008-01-08 14:58:56 -0500},
4087 Date-Modified = {2008-01-08 14:59:03 -0500},
4088 Journal = prl,
4089 Pages = 295,
4090 Volume = 71,
4091 Year = 1993}
4092
4093 @article{Egelhoff89,
4094 Author = {W.~F. Egelhoff and I. Jacob},
4095 Date-Added = {2008-01-08 14:58:56 -0500},
4096 Date-Modified = {2008-01-08 14:59:03 -0500},
4097 Journal = prl,
4098 Pages = 921,
4099 Volume = 62,
4100 Year = 1989}
4101
4102 @article{Dobson1987,
4103 Author = {B.~W. Dobson},
4104 Date-Added = {2008-01-08 14:58:56 -0500},
4105 Date-Modified = {2008-01-08 14:59:03 -0500},
4106 Journal = prb,
4107 Pages = 1068,
4108 Volume = 36,
4109 Year = 1987}
4110
4111 @article{Davis:1969uq,
4112 Abstract = { Exact solutions of the Stokes equations are derived for the case of two unequal spheres slowly rotating or translating perpendicular to their line of centers in a quiescent, unbounded viscous fluid, following Wakiya[16]. Numerical results are presented for the force and torque coefficients for size ratios from 1[middle dot]0 to 10[middle dot]0, and separations down to 0[middle dot]001 times the radius of the smaller.},
4113 Author = {Davis, M. H.},
4114 Date-Added = {2008-01-08 14:57:14 -0500},
4115 Date-Modified = {2008-01-08 14:57:14 -0500},
4116 Journal = {Chemical Engineering Science},
4117 Number = 12,
4118 Pages = {1769--1776},
4119 Title = {The slow translation and rotation of two unequal spheres in a viscous fluid},
4120 Ty = {JOUR},
4121 Url = {http://www.sciencedirect.com/science/article/B6TFK-445H8BM-84/2/b34951283900cdde792ec1309ec51565},
4122 Volume = 24,
4123 Year = 1969,
4124 Bdsk-Url-1 = {http://www.sciencedirect.com/science/article/B6TFK-445H8BM-84/2/b34951283900cdde792ec1309ec51565}}
4125
4126 @article{Stimson:1926qy,
4127 Author = {Stimson, M and Jeffery, GB},
4128 Date-Added = {2008-01-08 14:51:23 -0500},
4129 Date-Modified = {2008-01-08 14:51:35 -0500},
4130 Journal = {Proceedings of the Royal Society of London Series A-Containing Papers of a Mathematical and Physical Character},
4131 Pages = {110-116},
4132 Title = {The motion of two spheres in a viscous fluid},
4133 Volume = 111,
4134 Year = 1926}
4135
4136 @article{Orlandi:2006fk,
4137 Abstract = {Liquid crystal phases formed by bent-shaped (or {\tt{}"{}}banana{\tt{}"{}}) molecules are currently of great interest. Here we investigate by Monte Carlo computer simulations the phases formed by rigid banana molecules modeled combining three Gay-Berne sites and containing either one central or two lateral and transversal dipoles. We show that changing the dipole position and orientation has a profound effect on the mesophase stability and molecular organization. In particular, we find a uniaxial nematic phase only for off-center dipolar models and tilted phases only for the one with terminal dipoles.},
4138 Address = {Dipartimento di Chimica Fisica e Inorganica, and INSTM, Universita di Bologna, Viale Risorgimento 4, 40136 Bologna, Italy.},
4139 Au = {Orlandi, S and Berardi, R and Steltzer, J and Zannoni, C},
4140 Author = {Orlandi, Silvia and Berardi, Roberto and Steltzer, Joachim and Zannoni, Claudio},
4141 Da = 20060407,
4142 Date-Added = {2008-01-08 14:47:56 -0500},
4143 Date-Modified = {2008-01-08 14:48:06 -0500},
4144 Dcom = 20070727,
4145 Doi = {10.1063/1.2176622},
4146 Edat = {2006/04/08 09:00},
4147 Issn = {0021-9606 (Print)},
4148 Jid = 0375360,
4149 Journal = {J Chem Phys},
4150 Jt = {The Journal of chemical physics},
4151 Language = {eng},
4152 Mhda = {2006/04/08 09:01},
4153 Number = 12,
4154 Own = {NLM},
4155 Pages = 124907,
4156 Pl = {United States},
4157 Pmid = 16599725,
4158 Pst = {ppublish},
4159 Pt = {Journal Article},
4160 Pubm = {Print},
4161 So = {J Chem Phys. 2006 Mar 28;124(12):124907.},
4162 Stat = {PubMed-not-MEDLINE},
4163 Title = {A Monte Carlo study of the mesophases formed by polar bent-shaped molecules.},
4164 Volume = 124,
4165 Year = 2006,
4166 Bdsk-Url-1 = {http://dx.doi.org/10.1063/1.2176622}}
4167
4168 @article{sun:031602,
4169 Author = {Xiuquan Sun and J. Daniel Gezelter},
4170 Date-Added = {2008-01-08 14:42:33 -0500},
4171 Date-Modified = {2008-01-08 14:42:33 -0500},
4172 Doi = {10.1103/PhysRevE.75.031602},
4173 Eid = 031602,
4174 Journal = {Physical Review E (Statistical, Nonlinear, and Soft Matter Physics)},
4175 Keywords = {lattice theory; membranes},
4176 Number = 3,
4177 Numpages = 7,
4178 Pages = 031602,
4179 Publisher = {APS},
4180 Title = {Spontaneous corrugation of dipolar membranes},
4181 Url = {http://link.aps.org/abstract/PRE/v75/e031602},
4182 Volume = 75,
4183 Year = 2007,
4184 Bdsk-Url-1 = {http://link.aps.org/abstract/PRE/v75/e031602},
4185 Bdsk-Url-2 = {http://dx.doi.org/10.1103/PhysRevE.75.031602}}
4186
4187 @article{Ortega:2007lr,
4188 Abstract = {The equivalent radius for any solution property is the radius of a spherical particle having the same value of solution property as that of the macromolecule under consideration. Equivalent radii for different properties present a dependence on size and shape that are more similar than the values of the properties themselves. Furthermore, the ratios of equivalent radii of two properties depend on the conformation (shape or flexibility), but not on the absolute sizes. We define equivalent radii and their ratios, and describe their evaluation for some common models of rigid and flexible macromolecules. Using radii and ratios, we have devised procedures to fit macromolecular models to experimental properties, allowing the determination of the model parameters. Using these quantities, we can construct target functions for an equilibrated, unbiased optimization. The procedures, which have been implemented in public-domain computer programs, are illustrated for rigid, globular proteins, and the rodlike tobacco mosaic virus, and for semiflexible, wormlike heparin molecules.},
4189 Address = {Departamento de Quimica Fisica, Facultad de Quimica, Universidad de Murcia, 30071 Murcia, Spain.},
4190 Au = {Ortega, A and {Garc\'{i}a de la Torre}, Jose},
4191 Author = {Ortega, A and {Garc\'{i}a de la Torre}, Jose},
4192 Da = 20070813,
4193 Date-Added = {2008-01-08 14:38:03 -0500},
4194 Date-Modified = {2008-01-08 14:38:49 -0500},
4195 Dcom = 20071017,
4196 Dep = 20070724,
4197 Doi = {10.1021/bm700473f},
4198 Edat = {2007/07/25 09:00},
4199 Issn = {1525-7797 (Print)},
4200 Jid = 100892849,
4201 Journal = {Biomacromolecules},
4202 Jt = {Biomacromolecules},
4203 Keywords = {Computer Simulation; Heparin/chemistry; Macromolecular Substances/*chemistry; *Models, Chemical; *Models, Molecular; Molecular Conformation; Particle Size; Protein Conformation; Proteins/chemistry; Software; Solutions},
4204 Language = {eng},
4205 Mhda = {2007/10/18 09:00},
4206 Number = 8,
4207 Own = {NLM},
4208 Pages = {2464--2475},
4209 Phst = {2007/07/24 {$[$}aheadofprint{$]$}},
4210 Pl = {United States},
4211 Pmid = 17645309,
4212 Pst = {ppublish},
4213 Pt = {Journal Article; Research Support, Non-U.S. Gov't},
4214 Pubm = {Print-Electronic},
4215 Rn = {0 (Macromolecular Substances); 0 (Proteins); 0 (Solutions); 9005-49-6 (Heparin)},
4216 Sb = {IM},
4217 So = {Biomacromolecules. 2007 Aug;8(8):2464-75. Epub 2007 Jul 24.},
4218 Stat = {MEDLINE},
4219 Title = {Equivalent radii and ratios of radii from solution properties as indicators of macromolecular conformation, shape, and flexibility.},
4220 Volume = 8,
4221 Year = 2007,
4222 Bdsk-Url-1 = {http://dx.doi.org/10.1021/bm700473f}}
4223
4224 @article{Torre2003,
4225 Abstract = {While the prediction of hydrodynamic properties of rigid particles
4226 is nowadays feasible using simple and efficient computer programs,
4227 the calculation of such properties and, in general, the dynamic
4228 behavior of flexible macromolecules has not reached a similar situation.
4229 Although the theories are available, usually the computational work
4230 is done using solutions specific for each problem. We intend to
4231 develop computer programs that would greatly facilitate the task
4232 of predicting solution behavior of flexible macromolecules. In this
4233 paper, we first present an overview of the two approaches that are
4234 most practical: the Monte Carlo rigid-body treatment, and the Brownian
4235 dynamics simulation technique. The Monte Carlo procedure is based
4236 on the calculation of properties for instantaneous conformations
4237 of the macromolecule that are regarded as if they were instantaneously
4238 rigid. We describe how a Monte Carlo program can be interfaced to
4239 the programs in the HYDRO suite for rigid particles, and provide
4240 an example of such calculation, for a hypothetical particle: a protein
4241 with two domains connected by a flexible linker. We also describe
4242 briefly the essentials of Brownian dynamics, and propose a general
4243 mechanical model that includes several kinds of intramolecular interactions,
4244 such as bending, internal rotation, excluded volume effects, etc.
4245 We provide an example of the application of this methodology to
4246 the dynamics of a semiflexible, wormlike DNA.},
4247 Annote = {724XK Times Cited:6 Cited References Count:64},
4248 Author = {{Garc\'{i}a de la Torre}, Jose and H. E. Sanchez and A. Ortega and J. G. Hernandez and M. X. Fernandes and F. G. Diaz and M. C. L. Martinez},
4249 Issn = {0175-7571},
4250 Journal = {European Biophysics Journal with Biophysics Letters},
4251 Month = {Aug},
4252 Number = 5,
4253 Pages = {477-486},
4254 Title = {Calculation of the solution properties of flexible macromolecules: methods and applications},
4255 Uri = {<Go to ISI>://000185513400011},
4256 Volume = 32,
4257 Year = 2003}
4258
4259 @article{Alakent2005,
4260 Abstract = {Time series analysis tools are employed on the principal modes obtained
4261 from the C-alpha trajectories from two independent molecular-dynamics
4262 simulations of alpha-amylase inhibitor (tendamistat). Fluctuations
4263 inside an energy minimum (intraminimum motions), transitions between
4264 minima (interminimum motions), and relaxations in different hierarchical
4265 energy levels are investigated and compared with those encountered
4266 in vacuum by using different sampling window sizes and intervals.
4267 The low-frequency low-indexed mode relationship, established in
4268 vacuum, is also encountered in water, which shows the reliability
4269 of the important dynamics information offered by principal components
4270 analysis in water. It has been shown that examining a short data
4271 collection period (100 ps) may result in a high population of overdamped
4272 modes, while some of the low-frequency oscillations (< 10 cm(-1))
4273 can be captured in water by using a longer data collection period
4274 (1200 ps). Simultaneous analysis of short and long sampling window
4275 sizes gives the following picture of the effect of water on protein
4276 dynamics. Water makes the protein lose its memory: future conformations
4277 are less dependent on previous conformations due to the lowering
4278 of energy barriers in hierarchical levels of the energy landscape.
4279 In short-time dynamics (< 10 ps), damping factors extracted from
4280 time series model parameters are lowered. For tendamistat, the friction
4281 coefficient in the Langevin equation is found to be around 40-60
4282 cm(-1) for the low-indexed modes, compatible with literature. The
4283 fact that water has increased the friction and that on the other
4284 hand has lubrication effect at first sight contradicts. However,
4285 this comes about because water enhances the transitions between
4286 minima and forces the protein to reduce its already inherent inability
4287 to maintain oscillations observed in vacuum. Some of the frequencies
4288 lower than 10 cm(-1) are found to be overdamped, while those higher
4289 than 20 cm(-1) are slightly increased. As for the long-time dynamics
4290 in water, it is found that random-walk motion is maintained for
4291 approximately 200 ps (about five times of that in vacuum) in the
4292 low-indexed modes, showing the lowering of energy barriers between
4293 the higher-level minima.},
4294 Annote = {973OH Times Cited:1 Cited References Count:33},
4295 Author = {B. Alakent and M. C. Camurdan and P. Doruker},
4296 Issn = {0021-9606},
4297 Journal = jcp,
4298 Month = {Oct 8},
4299 Number = 14,
4300 Pages = {-},
4301 Title = {Hierarchical structure of the energy landscape of proteins revisited by time series analysis. II. Investigation of explicit solvent effects},
4302 Uri = {<Go to ISI>://000232532000064},
4303 Volume = 123,
4304 Year = 2005}
4305
4306 @book{Alexander1987,
4307 Address = {New York},
4308 Author = {C. Alexander},
4309 Publisher = {Oxford University Press},
4310 Title = {A Pattern Language: Towns, Buildings, Construction},
4311 Year = 1987}
4312
4313 @book{Allen1987,
4314 Address = {New York},
4315 Author = {M.~P. Allen and D.~J. Tildesley},
4316 Publisher = {Oxford University Press},
4317 Title = {Computer Simulations of Liquids},
4318 Year = 1987}
4319
4320 @article{Allison1991,
4321 Abstract = {A Brownian dynamics algorithm is developed to simulate dynamics experiments
4322 of rigid macromolecules. It is applied to polarized dynamic light
4323 scattering from rodlike sturctures and from a model of a DNA fragment
4324 (762 base pairs). A number of rod cases are examined in which the
4325 translational anisotropy is increased form zero to a large value.
4326 Simulated first cumulants as well as amplitudes and lifetimes of
4327 the dynamic form factor are compared with predictions of analytic
4328 theories and found to be in very good agreement with them. For DNA
4329 fragments 762 base pairs in length or longer, translational anisotropy
4330 does not contribute significantly to dynamic light scattering. In
4331 a comparison of rigid and flexible simulations on semistiff models
4332 of this fragment, it is shown directly that flexing contributes
4333 to the faster decay processes probed by light scattering and that
4334 the flexible model studies are in good agreement with experiment.},
4335 Annote = {Eu814 Times Cited:8 Cited References Count:32},
4336 Author = {S. A. Allison},
4337 Issn = {0024-9297},
4338 Journal = {Macromolecules},
4339 Month = {Jan 21},
4340 Number = 2,
4341 Pages = {530-536},
4342 Title = {A Brownian Dynamics Algorithm for Arbitrary Rigid Bodies - Application to Polarized Dynamic Light-Scattering},
4343 Uri = {<Go to ISI>://A1991EU81400029},
4344 Volume = 24,
4345 Year = 1991}
4346
4347 @article{Andersen1983,
4348 Annote = {Rq238 Times Cited:559 Cited References Count:14},
4349 Author = {H. C. Andersen},
4350 Issn = {0021-9991},
4351 Journal = jcop,
4352 Number = 1,
4353 Pages = {24-34},
4354 Title = {Rattle - a Velocity Version of the Shake Algorithm for Molecular-Dynamics Calculations},
4355 Uri = {<Go to ISI>://A1983RQ23800002},
4356 Volume = 52,
4357 Year = 1983}
4358
4359 @article{Auerbach2005,
4360 Abstract = {Acetylcholine receptor channels (AChRs) are proteins that switch between
4361 stable #closed# and #open# conformations. In patch clamp recordings,
4362 diliganded AChR gating appears to be a simple, two-state reaction.
4363 However, mutagenesis studies indicate that during gating dozens
4364 of residues across the protein move asynchronously and are organized
4365 into rigid body gating domains (#blocks#). Moreover, there is an
4366 upper limit to the apparent channel opening rate constant. These
4367 observations suggest that the gating reaction has a broad, corrugated
4368 transition state region, with the maximum opening rate reflecting,
4369 in part, the mean first-passage time across this ensemble. Simulations
4370 reveal that a flat, isotropic energy profile for the transition
4371 state can account for many of the essential features of AChR gating.
4372 With this mechanism, concerted, local structural transitions that
4373 occur on the broad transition state ensemble give rise to fractional
4374 measures of reaction progress (Phi values) determined by rate-equilibrium
4375 free energy relationship analysis. The results suggest that the
4376 coarse-grained AChR gating conformational change propagates through
4377 the protein with dynamics that are governed by the Brownian motion
4378 of individual gating blocks.},
4379 Annote = {895QF Times Cited:9 Cited References Count:33},
4380 Author = {A. Auerbach},
4381 Issn = {0027-8424},
4382 Journal = pnas,
4383 Month = {Feb 1},
4384 Number = 5,
4385 Pages = {1408-1412},
4386 Title = {Gating of acetylcholine receptor channels: Brownian motion across a broad transition state},
4387 Uri = {<Go to ISI>://000226877300030},
4388 Volume = 102,
4389 Year = 2005}
4390
4391 @article{Baber1995,
4392 Abstract = {The effect of the general anesthetics halothane, enflurane, and isoflurane
4393 on hydrocarbon chain packing in palmitoyl(d(31))oleoylphosphatidylcholine
4394 membranes in the liquid crystalline phase was investigated using
4395 H-2 NMR. Upon the addition of the anesthetics, the first five methylene
4396 units near the interface generally show a very small increase in
4397 segmental order, while segments deeper within the bilayer show a
4398 small decrease in segmental order. From the H-2 NMR results, the
4399 chain length for the perdeuterated palmitoyl chain in the absence
4400 of anesthetic was found to be 12.35 Angstrom. Upon the addition
4401 of halothane enflurane, or isoflurane, the acyl chain undergoes
4402 slight contractions of 0.11, 0.20, or 0.16 Angstrom, respectively,
4403 at 50 mol % anesthetic. A simple model was used to estimate the
4404 relative amounts of anesthetic located near the interface and deeper
4405 in the bilayer hydrocarbon region, and only a slight preference
4406 for an interfacial location was observed. Intermolecular H-1-H-1
4407 nuclear Overhauser effects (NOEs) were measured between phospholipid
4408 and halothane protons. These NOEs are consistent with the intramembrane
4409 location of the anesthetics suggested by the H-2 NMR data. In addition,
4410 the NOE data indicate that anesthetics prefer the interfacial and
4411 hydrocarbon regions of the membrane and are not found in high concentrations
4412 in the phospholipid headgroup.},
4413 Annote = {Qz716 Times Cited:38 Cited References Count:37},
4414 Author = {J. Baber and J. F. Ellena and D. S. Cafiso},
4415 Issn = {0006-2960},
4416 Journal = {Biochemistry},
4417 Month = {May 16},
4418 Number = 19,
4419 Pages = {6533-6539},
4420 Title = {Distribution of General-Anesthetics in Phospholipid-Bilayers Determined Using H-2 Nmr and H-1-H-1 Noe Spectroscopy},
4421 Uri = {<Go to ISI>://A1995QZ71600035},
4422 Volume = 34,
4423 Year = 1995}
4424
4425 @article{Banerjee2004,
4426 Abstract = {Based on a coherent state representation of noise operator and an
4427 ensemble averaging procedure using Wigner canonical thermal distribution
4428 for harmonic oscillators, a generalized quantum Langevin equation
4429 has been recently developed [Phys. Rev. E 65, 021109 (2002); 66,
4430 051106 (2002)] to derive the equations of motion for probability
4431 distribution functions in c-number phase-space. We extend the treatment
4432 to explore several systematic approximation schemes for the solutions
4433 of the Langevin equation for nonlinear potentials for a wide range
4434 of noise correlation, strength and temperature down to the vacuum
4435 limit. The method is exemplified by an analytic application to harmonic
4436 oscillator for arbitrary memory kernel and with the help of a numerical
4437 calculation of barrier crossing, in a cubic potential to demonstrate
4438 the quantum Kramers' turnover and the quantum Arrhenius plot. (C)
4439 2004 American Institute of Physics.},
4440 Annote = {816YY Times Cited:8 Cited References Count:35},
4441 Author = {D. Banerjee and B. C. Bag and S. K. Banik and D. S. Ray},
4442 Issn = {0021-9606},
4443 Journal = jcp,
4444 Month = {May 15},
4445 Number = 19,
4446 Pages = {8960-8972},
4447 Title = {Solution of quantum Langevin equation: Approximations, theoretical and numerical aspects},
4448 Uri = {<Go to ISI>://000221146400009},
4449 Volume = 120,
4450 Year = 2004}
4451
4452 @article{Barojas1973,
4453 Author = {J. Barojas and D. Levesque},
4454 Journal = {Phys. Rev. A},
4455 Pages = {1092-1105},
4456 Title = {Simulation of Diatomic Homonuclear Liquids},
4457 Volume = 7,
4458 Year = 1973}
4459
4460 @article{Barth1998,
4461 Abstract = {We present an efficient new method termed LN for propagating biomolecular
4462 dynamics according to the Langevin equation that arose fortuitously
4463 upon analysis of the range of harmonic validity of our normal-mode
4464 scheme LIN. LN combines force linearization with force splitting
4465 techniques and disposes of LIN'S computationally intensive minimization
4466 (anharmonic correction) component. Unlike the competitive multiple-timestepping
4467 (MTS) schemes today-formulated to be symplectic and time-reversible-LN
4468 merges the slow and fast forces via extrapolation rather than impulses;
4469 the Langevin heat bath prevents systematic energy drifts. This combination
4470 succeeds in achieving more significant speedups than these MTS methods
4471 which are Limited by resonance artifacts to an outer timestep less
4472 than some integer multiple of half the period of the fastest motion
4473 (around 4-5 fs for biomolecules). We show that LN achieves very
4474 good agreement with small-timestep solutions of the Langevin equation
4475 in terms of thermodynamics (energy means and variances), geometry,
4476 and dynamics (spectral densities) for two proteins in vacuum and
4477 a large water system. Significantly, the frequency of updating the
4478 slow forces extends to 48 fs or more, resulting in speedup factors
4479 exceeding 10. The implementation of LN in any program that employs
4480 force-splitting computations is straightforward, with only partial
4481 second-derivative information required, as well as sparse Hessian/vector
4482 multiplication routines. The linearization part of LN could even
4483 be replaced by direct evaluation of the fast components. The application
4484 of LN to biomolecular dynamics is well suited for configurational
4485 sampling, thermodynamic, and structural questions. (C) 1998 American
4486 Institute of Physics.},
4487 Annote = {105HH Times Cited:29 Cited References Count:49},
4488 Author = {E. Barth and T. Schlick},
4489 Issn = {0021-9606},
4490 Journal = jcp,
4491 Month = {Aug 1},
4492 Number = 5,
4493 Pages = {1617-1632},
4494 Title = {Overcoming stability limitations in biomolecular dynamics. I. Combining force splitting via extrapolation with Langevin dynamics in LN},
4495 Uri = {<Go to ISI>://000075066300006},
4496 Volume = 109,
4497 Year = 1998}
4498
4499 @article{Batcho2001,
4500 Abstract = {We present an analysis for a simple two-component harmonic oscillator
4501 that compares the use of position-Verlet to velocity-Verlet for
4502 multiple-time step integration. The numerical stability analysis
4503 based on the impulse-Verlet splitting shows that position-Verlet
4504 has enhanced stability, in terms of the largest allowable time step,
4505 for cases where an ample separation of time scales exists. Numerical
4506 investigations confirm the advantages of the position-Verlet scheme
4507 when used for the fastest time scales of the system. Applications
4508 to a biomolecule. a solvated protein, for both Newtonian and Langevin
4509 dynamics echo these trends over large outer time-step regimes. (C)
4510 2001 American Institute of Physics.},
4511 Annote = {469KV Times Cited:6 Cited References Count:30},
4512 Author = {P. F. Batcho and T. Schlick},
4513 Issn = {0021-9606},
4514 Journal = jcp,
4515 Month = {Sep 1},
4516 Number = 9,
4517 Pages = {4019-4029},
4518 Title = {Special stability advantages of position-Verlet over velocity-Verlet in multiple-time step integration},
4519 Uri = {<Go to ISI>://000170813800005},
4520 Volume = 115,
4521 Year = 2001}
4522
4523 @article{Bates2005,
4524 Abstract = {Inspired by recent claims that compounds composed of V-shaped molecules
4525 can exhibit the elusive biaxial nematic phase, we have developed
4526 a generic simulation model for such systems. This contains the features
4527 of the molecule that are essential to its liquid crystal behavior,
4528 namely the anisotropies of the two arms and the angle between them.
4529 The behavior of the model has been investigated using Monte Carlo
4530 simulations for a wide range of these structural parameters. This
4531 allows us to establish the relationship between the V-shaped molecule
4532 and its ability to form a biaxial nematic phase. Of particular importance
4533 are the criteria of geometry and the relative anisotropy necessary
4534 for the system to exhibit a Landau point, at which the biaxial nematic
4535 is formed directly from the isotropic phase. The simulations have
4536 also been used to determine the orientational order parameters for
4537 a selection of molecular axes. These are especially important because
4538 they reveal the phase symmetry and are connected to the experimental
4539 determination of this. The simulation results show that, whereas
4540 some positions are extremely sensitive to the phase biaxiality,
4541 others are totally blind to this.},
4542 Annote = {Part 1 988LQ Times Cited:0 Cited References Count:38},
4543 Author = {M. A. Bates and G. R. Luckhurst},
4544 Issn = {1539-3755},
4545 Journal = {Physical Review E},
4546 Month = {Nov},
4547 Number = 5,
4548 Pages = {-},
4549 Title = {Biaxial nematic phases and V-shaped molecules: A Monte Carlo simulation study},
4550 Uri = {<Go to ISI>://000233603100030},
4551 Volume = 72,
4552 Year = 2005}
4553
4554 @article{Beard2003,
4555 Abstract = {We introduce an unbiased protocol for performing rotational moves
4556 in rigid-body dynamics simulations. This approach - based on the
4557 analytic solution for the rotational equations of motion for an
4558 orthogonal coordinate system at constant angular velocity - removes
4559 deficiencies that have been largely ignored in Brownian dynamics
4560 simulations, namely errors for finite rotations that result from
4561 applying the noncommuting rotational matrices in an arbitrary order.
4562 Our algorithm should thus replace standard approaches to rotate
4563 local coordinate frames in Langevin and Brownian dynamics simulations.},
4564 Annote = {736UA Times Cited:0 Cited References Count:11},
4565 Author = {D. A. Beard and T. Schlick},
4566 Issn = {0006-3495},
4567 Journal = bj,
4568 Month = {Nov 1},
4569 Number = 5,
4570 Pages = {2973-2976},
4571 Title = {Unbiased rotational moves for rigid-body dynamics},
4572 Uri = {<Go to ISI>://000186190500018},
4573 Volume = 85,
4574 Year = 2003}
4575
4576 @article{Beloborodov1998,
4577 Abstract = {Using the Green function of arbitrary rigid Brownian diffusion (Goldstein,
4578 Biopolymers 33, 409-436, 1993), it was analytically shown that coupling
4579 between translation and rotation diffusion degrees of freedom does
4580 not affect the correlation functions relevant to the NMR intramolecular
4581 relaxation. It follows that spectral densities usually used for
4582 the anisotropic rotation diffusion (Woessner, J. Chem. Phys. 37,
4583 647-654, 1962) can be regarded as exact in respect to the rotation-translation
4584 coupling for the spin system connected with a rigid body. (C) 1998
4585 Academic Press.},
4586 Annote = {Zu605 Times Cited:2 Cited References Count:6},
4587 Author = {I. S. Beloborodov and V. Y. Orekhov and A. S. Arseniev},
4588 Issn = {1090-7807},
4589 Journal = {Journal of Magnetic Resonance},
4590 Month = {Jun},
4591 Number = 2,
4592 Pages = {328-329},
4593 Title = {Effect of coupling between rotational and translational Brownian motions on NMR spin relaxation: Consideration using green function of rigid body diffusion},
4594 Uri = {<Go to ISI>://000074214800017},
4595 Volume = 132,
4596 Year = 1998}
4597
4598 @article{Berardi1996,
4599 Abstract = {We demonstrate that the overall molecular dipole organization in a
4600 smectic liquid crystal formed of polar molecules can be strongly
4601 influenced by the position of the dipole in the molecule. We study
4602 by large scale Monte Carlo simulations systems of attractive-repulsive
4603 ''Gay-Berne'' elongated ellipsoids with an axial dipole at the center
4604 or near the end of the molecule and we show that monolayer smectic
4605 liquid crystals and modulated antiferroelectric bilayer stripe domains
4606 similar to the experimentally observed ''antiphase'' structures
4607 are obtained in the two cases.},
4608 Annote = {Vn637 Times Cited:49 Cited References Count:26},
4609 Author = {R. Berardi and S. Orlandi and C. Zannoni},
4610 Issn = {0009-2614},
4611 Journal = {Chemical Physics Letters},
4612 Month = {Oct 18},
4613 Number = 3,
4614 Pages = {357-362},
4615 Title = {Antiphase structures in polar smectic liquid crystals and their molecular origin},
4616 Uri = {<Go to ISI>://A1996VN63700023},
4617 Volume = 261,
4618 Year = 1996}
4619
4620 @article{Berkov2005,
4621 Abstract = {In this paper a detailed numerical study (in frames of the Slonczewski
4622 formalism) of magnetization oscillations driven by a spin-polarized
4623 current through a thin elliptical nanoelement is presented. We show
4624 that a sophisticated micromagnetic model, where a polycrystalline
4625 structure of a nanoelement is taken into account, can explain qualitatively
4626 all most important features of the magnetization oscillation spectra
4627 recently observed experimentally [S. I. Kiselev , Nature 425, 380
4628 (2003)], namely, existence of several equidistant spectral bands,
4629 sharp onset and abrupt disappearance of magnetization oscillations
4630 with increasing current, absence of the out-of-plane regime predicted
4631 by a macrospin model, and the relation between frequencies of so-called
4632 small-angle and quasichaotic oscillations. However, a quantitative
4633 agreement with experimental results (especially concerning the frequency
4634 of quasichaotic oscillations) could not be achieved in the region
4635 of reasonable parameter values, indicating that further model refinement
4636 is necessary for a complete understanding of the spin-driven magnetization
4637 precession even in this relatively simple experimental situation.},
4638 Annote = {969IT Times Cited:2 Cited References Count:55},
4639 Author = {D. V. Berkov and N. L. Gorn},
4640 Issn = {1098-0121},
4641 Journal = {Physical Review B},
4642 Month = {Sep},
4643 Number = 9,
4644 Pages = {-},
4645 Title = {Magnetization precession due to a spin-polarized current in a thin nanoelement: Numerical simulation study},
4646 Uri = {<Go to ISI>://000232228500058},
4647 Volume = 72,
4648 Year = 2005}
4649
4650 @article{Berkov2005a,
4651 Abstract = {Numerical simulations of fast remagnetization processes using stochastic
4652 dynamics are widely used to study various magnetic systems. In this
4653 paper, we first address several crucial methodological problems
4654 of such simulations: (i) the influence of finite-element discretization
4655 on simulated dynamics, (ii) choice between Ito and Stratonovich
4656 stochastic calculi by the solution of micromagnetic stochastic equations
4657 of motion and (iii) non-trivial correlation properties of the random
4658 (thermal) field. Next, we discuss several examples to demonstrate
4659 the great potential of the Langevin dynamics for studying fast remagnetization
4660 processes in technically relevant applications: we present numerical
4661 analysis of equilibrium magnon spectra in patterned structures,
4662 study thermal noise effects on the magnetization dynamics of nanoelements
4663 in pulsed fields and show some results for a remagnetization dynamics
4664 induced by a spin-polarized current. (c) 2004 Elsevier B.V. All
4665 rights reserved.},
4666 Annote = {Part 1 Sp. Iss. SI 922KU Times Cited:2 Cited References Count:25},
4667 Author = {D. V. Berkov and N. L. Gorn},
4668 Issn = {0304-8853},
4669 Journal = {Journal of Magnetism and Magnetic Materials},
4670 Month = {Apr},
4671 Pages = {442-448},
4672 Title = {Stochastic dynamic simulations of fast remagnetization processes: recent advances and applications},
4673 Uri = {<Go to ISI>://000228837600109},
4674 Volume = 290,
4675 Year = 2005}
4676
4677 @article{Berkov2002,
4678 Abstract = {We report on recent progress achieved by the development of numerical
4679 methods based on the stochastic (Langevin) dynamics applied to systems
4680 of interacting magnetic nanoparticles. The method enables direct
4681 simulations of the trajectories of magnetic moments taking into
4682 account (i) all relevant interactions, (ii) precession dynamics,
4683 and (iii) temperature fluctuations included via the random (thermal)
4684 field. We present several novel results obtained using new methods
4685 developed for the solution of the Langevin equations. In particular,
4686 we have investigated magnetic nanodots and disordered granular systems
4687 of single-domain magnetic particles. For the first case we have
4688 calculated the spectrum and the spatial distribution of spin excitations.
4689 For the second system the complex ac susceptibility chi(omega, T)
4690 for various particle concentrations and particle anisotropies were
4691 computed and compared with numerous experimental results.},
4692 Annote = {526TF Times Cited:4 Cited References Count:37},
4693 Author = {D. V. Berkov and N. L. Gorn and P. Gornert},
4694 Issn = {0031-8965},
4695 Journal = {Physica Status Solidi a-Applied Research},
4696 Month = {Feb 16},
4697 Number = 2,
4698 Pages = {409-421},
4699 Title = {Magnetization dynamics in nanoparticle systems: Numerical simulation using Langevin dynamics},
4700 Uri = {<Go to ISI>://000174145200026},
4701 Volume = 189,
4702 Year = 2002}
4703
4704 @article{Bernal1980,
4705 Author = {J.M. Bernal and {Garc\'{i}a de la Torre}, Jose},
4706 Journal = {Biopolymers},
4707 Pages = {751-766},
4708 Title = {Transport Properties and Hydrodynamic Centers of Rigid Macromolecules with Arbitrary Shape},
4709 Volume = 19,
4710 Year = 1980}
4711
4712 @article{Brenner1967,
4713 Author = {H. Brenner},
4714 Journal = {J. Collid. Int. Sci.},
4715 Pages = {407-436},
4716 Title = {Coupling between the Translational and Rotational Brownian Motions of Rigid Particles of Arbitrary shape},
4717 Volume = 23,
4718 Year = 1967}
4719
4720 @article{Brooks1983,
4721 Annote = {Qp423 Times Cited:6414 Cited References Count:96},
4722 Author = {B. R. Brooks and R. E. Bruccoleri and B. D. Olafson and D. J. States and S. Swaminathan and M. Karplus},
4723 Issn = {0192-8651},
4724 Journal = jcc,
4725 Number = 2,
4726 Pages = {187-217},
4727 Title = {Charmm - a Program for Macromolecular Energy, Minimization, and Dynamics Calculations},
4728 Uri = {<Go to ISI>://A1983QP42300010},
4729 Volume = 4,
4730 Year = 1983}
4731
4732 @article{Brunger1984,
4733 Annote = {Sm173 Times Cited:143 Cited References Count:22},
4734 Author = {A. Brunger and C. L. Brooks and M. Karplus},
4735 Issn = {0009-2614},
4736 Journal = {Chemical Physics Letters},
4737 Number = 5,
4738 Pages = {495-500},
4739 Title = {Stochastic Boundary-Conditions for Molecular-Dynamics Simulations of St2 Water},
4740 Uri = {<Go to ISI>://A1984SM17300007},
4741 Volume = 105,
4742 Year = 1984}
4743
4744 @article{Budd1999,
4745 Abstract = {This paper examines a synthesis of adaptive mesh methods with the
4746 use of symmetry to study a partial differential equation. In particular,
4747 it considers methods which admit discrete self-similar solutions,
4748 examining the convergence of these to the true self-similar solution
4749 as well as their stability. Special attention is given to the nonlinear
4750 diffusion equation describing flow in a porous medium.},
4751 Annote = {199EE Times Cited:4 Cited References Count:14},
4752 Author = {C. J. Budd and G. J. Collins and W. Z. Huang and R. D. Russell},
4753 Issn = {1364-503X},
4754 Journal = {Philosophical Transactions of the Royal Society of London Series a-Mathematical Physical and Engineering Sciences},
4755 Month = {Apr 15},
4756 Number = 1754,
4757 Pages = {1047-1077},
4758 Title = {Self-similar numerical solutions of the porous-medium equation using moving mesh methods},
4759 Uri = {<Go to ISI>://000080466800005},
4760 Volume = 357,
4761 Year = 1999}
4762
4763 @article{Camp1999,
4764 Abstract = {Fluids of hard bent-core molecules have been studied using theory
4765 and computer simulation. The molecules are composed of two hard
4766 spherocylinders, with length-to-breadth ratio L/D, joined by their
4767 ends at an angle 180 degrees - gamma. For L/D = 2 and gamma = 0,10,20
4768 degrees, the simulations show isotropic, nematic, smectic, and solid
4769 phases. For L/D = 2 and gamma = 30 degrees, only isotropic, nematic,
4770 and solid phases are in evidence, which suggests that there is a
4771 nematic-smectic-solid triple point at an angle in the range 20 degrees
4772 < gamma < 30 degrees. In all of the orientationally ordered fluid
4773 phases the order is purely uniaxial. For gamma = 10 degrees and
4774 20 degrees, at the studied densities, the solid is also uniaxially
4775 ordered, whilst for gamma = 30 degrees the solid layers are biaxially
4776 ordered. For L/D = 2 and gamma = 60 degrees and 90 degrees we find
4777 no spontaneous orientational ordering. This is shown to be due to
4778 the interlocking of dimer pairs which precludes alignment. We find
4779 similar results for L/D = 9.5 and gamma = 72 degrees, where an isotropic-biaxial
4780 nematic transition is predicted by Onsager theory. Simulations in
4781 the biaxial nematic phase show it to be at least mechanically stable
4782 with respect to the isotropic phase, however. We have compared the
4783 quasi-exact simulation results in the isotropic phase with the predicted
4784 equations of state from three theories: the virial expansion containing
4785 the second and third virial coefficients; the Parsons-Lee equation
4786 of state; an application of Wertheim's theory of associating fluids
4787 in the limit of infinite attractive association energy. For all
4788 of the molecule elongations and geometries we have simulated, the
4789 Wertheim theory proved to be the most accurate. Interestingly, the
4790 isotropic equation of state is virtually independent of the dimer
4791 bond angle-a feature that is also reflected in the lack of variation
4792 with angle of the calculated second and third virial coefficients.
4793 (C) 1999 American Institute of Physics. [S0021-9606(99)50445-5].},
4794 Annote = {255TC Times Cited:24 Cited References Count:38},
4795 Author = {P. J. Camp and M. P. Allen and A. J. Masters},
4796 Issn = {0021-9606},
4797 Journal = jcp,
4798 Month = {Dec 1},
4799 Number = 21,
4800 Pages = {9871-9881},
4801 Title = {Theory and computer simulation of bent-core molecules},
4802 Uri = {<Go to ISI>://000083685400056},
4803 Volume = 111,
4804 Year = 1999}
4805
4806 @article{Care2005,
4807 Abstract = {A review is presented of molecular and mesoscopic computer simulations
4808 of liquid crystalline systems. Molecular simulation approaches applied
4809 to such systems are described, and the key findings for bulk phase
4810 behaviour are reported. Following this, recently developed lattice
4811 Boltzmann approaches to the mesoscale modelling of nemato-dynanics
4812 are reviewed. This paper concludes with a discussion of possible
4813 areas for future development in this field.},
4814 Annote = {989TU Times Cited:2 Cited References Count:258},
4815 Author = {C. M. Care and D. J. Cleaver},
4816 Issn = {0034-4885},
4817 Journal = {Reports on Progress in Physics},
4818 Month = {Nov},
4819 Number = 11,
4820 Pages = {2665-2700},
4821 Title = {Computer simulation of liquid crystals},
4822 Uri = {<Go to ISI>://000233697600004},
4823 Volume = 68,
4824 Year = 2005}
4825
4826 @article{Carrasco1999,
4827 Abstract = {The hydrodynamic properties of rigid particles are calculated from
4828 models composed of spherical elements (beads) using theories developed
4829 by Kirkwood, Bloomfield, and their coworkers. Bead models have usually
4830 been built in such a way that the beads fill the volume occupied
4831 by the particles. Sometimes the beads are few and of varying sizes
4832 (bead models in the strict sense), and other times there are many
4833 small beads (filling models). Because hydrodynamic friction takes
4834 place at the molecular surface, another possibility is to use shell
4835 models, as originally proposed by Bloomfield. In this work, we have
4836 developed procedures to build models of the various kinds, and we
4837 describe the theory and methods for calculating their hydrodynamic
4838 properties, including approximate methods that may be needed to
4839 treat models with a very large number of elements. By combining
4840 the various possibilities of model building and hydrodynamic calculation,
4841 several strategies can be designed. We have made a quantitative
4842 comparison of the performance of the various strategies by applying
4843 them to some test cases, for which the properties are known a priori.
4844 We provide guidelines and computational tools for bead modeling.},
4845 Annote = {200TT Times Cited:46 Cited References Count:57},
4846 Author = {B. Carrasco and {Garc\'{i}a de la Torre}, Jose},
4847 Issn = {0006-3495},
4848 Journal = bj,
4849 Month = {Jun},
4850 Number = 6,
4851 Pages = {3044-3057},
4852 Title = {Hydrodynamic properties of rigid particles: Comparison of different modeling and computational procedures},
4853 Uri = {<Go to ISI>://000080556700016},
4854 Volume = 76,
4855 Year = 1999}
4856
4857 @article{Chandra1999,
4858 Abstract = {Dynamical properties of the soft sticky dipole (SSD) model of water
4859 are calculated by means of molecular dynamics simulations. Since
4860 this is not a simple point model, the forces and torques arising
4861 from the SSD potential are derived here. Simulations are carried
4862 out in the microcanonical ensemble employing the Ewald method for
4863 the electrostatic interactions. Various time correlation functions
4864 and dynamical quantities associated with the translational and rotational
4865 motion of water molecules are evaluated and compared with those
4866 of two other commonly used models of liquid water, namely the transferable
4867 intermolecular potential-three points (TIP3P) and simple point charge/extended
4868 (SPC/E) models, and also with experiments. The dynamical properties
4869 of the SSD water model are found to be in good agreement with the
4870 experimental results and appear to be better than the TIP3P and
4871 SPC/E models in most cases, as has been previously shown for its
4872 thermodynamic, structural, and dielectric properties. Also, molecular
4873 dynamics simulations of the SSD model are found to run much faster
4874 than TIP3P, SPC/E, and other multisite models. (C) 1999 American
4875 Institute of Physics. [S0021-9606(99)51430-X].},
4876 Annote = {221EN Times Cited:14 Cited References Count:66},
4877 Author = {A. Chandra and T. Ichiye},
4878 Issn = {0021-9606},
4879 Journal = jcp,
4880 Month = {Aug 8},
4881 Number = 6,
4882 Pages = {2701-2709},
4883 Title = {Dynamical properties of the soft sticky dipole model of water: Molecular dynamics simulations},
4884 Uri = {<Go to ISI>://000081711200038},
4885 Volume = 111,
4886 Year = 1999}
4887
4888 @article{Channell1990,
4889 Annote = {Dk631 Times Cited:152 Cited References Count:34},
4890 Author = {P. J. Channell and C. Scovel},
4891 Issn = {0951-7715},
4892 Journal = {Nonlinearity},
4893 Month = {may},
4894 Number = 2,
4895 Pages = {231-259},
4896 Title = {Symplectic Integration of Hamiltonian-Systems},
4897 Uri = {<Go to ISI>://A1990DK63100001},
4898 Volume = 3,
4899 Year = 1990}
4900
4901 @article{Chen2003,
4902 Abstract = {We investigate the asymptotic behavior of systems of nonlinear differential
4903 equations and introduce a family of mixed methods from combinations
4904 of explicit Runge-Kutta methods. These methods have better stability
4905 behavior than traditional Runge-Kutta methods and generally extend
4906 the range of validity of the calculated solutions. These methods
4907 also give a way of determining if the numerical solutions are real
4908 or spurious. Emphasis is put on examples coming from mathematical
4909 models in ecology. (C) 2002 IMACS. Published by Elsevier Science
4910 B.V. All rights reserved.},
4911 Annote = {633ZD Times Cited:0 Cited References Count:9},
4912 Author = {B. Chen and F. Solis},
4913 Issn = {0168-9274},
4914 Journal = {Applied Numerical Mathematics},
4915 Month = {Jan},
4916 Number = {1-2},
4917 Pages = {21-30},
4918 Title = {Explicit mixed finite order Runge-Kutta methods},
4919 Uri = {<Go to ISI>://000180314200002},
4920 Volume = 44,
4921 Year = 2003}
4922
4923 @article{Cheung2004,
4924 Abstract = {Equilibrium molecular dynamics calculations have been performed for
4925 the liquid crystal molecule n-4-(trans-4-n-pentylcyclohexyl)benzonitrile
4926 (PCH5) using a fully atomistic model. Simulation data have been
4927 obtained for a series of temperatures in the nematic phase. The
4928 simulation data have been used to calculate the flexoelectric coefficients
4929 e(s) and e(b) using the linear response formalism of Osipov and
4930 Nemtsov [M. A. Osipov and V. B. Nemtsov, Sov. Phys. Crstallogr.
4931 31, 125 (1986)]. The temperature and order parameter dependence
4932 of e(s) and e(b) are examined, as are separate contributions from
4933 different intermolecular interactions. Values of e(s) and e(b) calculated
4934 from simulation are consistent with those found from experiment.
4935 (C) 2004 American Institute of Physics.},
4936 Annote = {866UM Times Cited:4 Cited References Count:61},
4937 Author = {D. L. Cheung and S. J. Clark and M. R. Wilson},
4938 Issn = {0021-9606},
4939 Journal = jcp,
4940 Month = {Nov 8},
4941 Number = 18,
4942 Pages = {9131-9139},
4943 Title = {Calculation of flexoelectric coefficients for a nematic liquid crystal by atomistic simulation},
4944 Uri = {<Go to ISI>://000224798900053},
4945 Volume = 121,
4946 Year = 2004}
4947
4948 @article{Cheung2002,
4949 Abstract = {Equilibrium molecular dynamics calculations have been performed for
4950 the liquid crystal molecule n-4-(trans-4-npentylcyclohexyl)benzonitrile
4951 (PCH5) using a fully atomistic model. Simulation data has been obtained
4952 for a series of temperatures in the nematic phase. The rotational
4953 viscosity co-efficient gamma(1), has been calculated using the angular
4954 velocity correlation function of the nematic director, n, the mean
4955 squared diffusion of n and statistical mechanical methods based
4956 on the rotational diffusion co-efficient. We find good agreement
4957 between the first two methods and experimental values. (C) 2002
4958 Published by Elsevier Science B.V.},
4959 Annote = {547KF Times Cited:8 Cited References Count:31},
4960 Author = {D. L. Cheung and S. J. Clark and M. R. Wilson},
4961 Issn = {0009-2614},
4962 Journal = {Chemical Physics Letters},
4963 Month = {Apr 15},
4964 Number = {1-2},
4965 Pages = {140-146},
4966 Title = {Calculation of the rotational viscosity of a nematic liquid crystal},
4967 Uri = {<Go to ISI>://000175331000020},
4968 Volume = 356,
4969 Year = 2002}
4970
4971 @article{Chin2004,
4972 Abstract = {Current molecular dynamics simulations of biomolecules using multiple
4973 time steps to update the slowly changing force are hampered by instabilities
4974 beginning at time steps near the half period of the fastest vibrating
4975 mode. These #resonance# instabilities have became a critical barrier
4976 preventing the long time simulation of biomolecular dynamics. Attempts
4977 to tame these instabilities by altering the slowly changing force
4978 and efforts to damp them out by Langevin dynamics do not address
4979 the fundamental cause of these instabilities. In this work, we trace
4980 the instability to the nonanalytic character of the underlying spectrum
4981 and show that a correct splitting of the Hamiltonian, which renders
4982 the spectrum analytic, restores stability. The resulting Hamiltonian
4983 dictates that in addition to updating the momentum due to the slowly
4984 changing force, one must also update the position with a modified
4985 mass. Thus multiple-time stepping must be done dynamically. (C)
4986 2004 American Institute of Physics.},
4987 Annote = {757TK Times Cited:1 Cited References Count:22},
4988 Author = {S. A. Chin},
4989 Issn = {0021-9606},
4990 Journal = jcp,
4991 Month = {Jan 1},
4992 Number = 1,
4993 Pages = {8-13},
4994 Title = {Dynamical multiple-time stepping methods for overcoming resonance instabilities},
4995 Uri = {<Go to ISI>://000187577400003},
4996 Volume = 120,
4997 Year = 2004}
4998
4999 @article{Cook2000,
5000 Abstract = {The Kirkwood correlation factor g(1) determines the preference for
5001 local parallel or antiparallel dipole association in the isotropic
5002 phase. Calamitic mesogens with longitudinal dipole moments and Kirkwood
5003 factors greater than 1 have an enhanced effective dipole moment
5004 along the molecular long axis. This leads to higher values of Delta
5005 epsilon in the nematic phase. This paper describes state-of-the-art
5006 molecular dynamics simulations of two calamitic mesogens 4-(trans-4-n-pentylcyclohexyl)benzonitrile
5007 (PCH5) and 4-(trans-4-n-pentylcyclohexyl) chlorobenzene (PCH5-Cl)
5008 in the isotropic liquid phase using an all-atom force field and
5009 taking long range electrostatics into account using an Ewald summation.
5010 Using this methodology, PCH5 is seen to prefer antiparallel dipole
5011 alignment with a negative g(1) and PCH5-Cl is seen to prefer parallel
5012 dipole alignment with a positive g(1); this is in accordance with
5013 experimental dielectric measurements. Analysis of the molecular
5014 dynamics trajectories allows an assessment of why these molecules
5015 behave differently.},
5016 Annote = {376BF Times Cited:10 Cited References Count:16},
5017 Author = {M. J. Cook and M. R. Wilson},
5018 Issn = {0267-8292},
5019 Journal = {Liquid Crystals},
5020 Month = {Dec},
5021 Number = 12,
5022 Pages = {1573-1583},
5023 Title = {Simulation studies of dipole correlation in the isotropic liquid phase},
5024 Uri = {<Go to ISI>://000165437800002},
5025 Volume = 27,
5026 Year = 2000}
5027
5028 @article{Cui2003,
5029 Abstract = {All-atom Langevin dynamics simulations have been performed to study
5030 the folding pathways of the 18-residue binding domain fragment E6ap
5031 of the human papillomavirus E6 interacting peptide. Six independent
5032 folding trajectories, with a total duration of nearly 2 mus, all
5033 lead to the same native state in which the E6ap adopts a fluctuating
5034 a-helix structure in the central portion (Ser-4-Leu-13) but with
5035 very flexible N and C termini. Simulations starting from different
5036 core configurations exhibit the E6ap folding dynamics as either
5037 a two- or three-state folder with an intermediate misfolded state.
5038 The essential leucine hydrophobic core (Leu-9, Leu-12, and Leu-13)
5039 is well conserved in the native-state structure but absent in the
5040 intermediate structure, suggesting that the leucine core is not
5041 only essential for the binding activity of E6ap but also important
5042 for the stability of the native structure. The free energy landscape
5043 reveals a significant barrier between the basins separating the
5044 native and misfolded states. We also discuss the various underlying
5045 forces that drive the peptide into its native state.},
5046 Annote = {689LC Times Cited:3 Cited References Count:48},
5047 Author = {B. X. Cui and M. Y. Shen and K. F. Freed},
5048 Issn = {0027-8424},
5049 Journal = pnas,
5050 Month = {Jun 10},
5051 Number = 12,
5052 Pages = {7087-7092},
5053 Title = {Folding and misfolding of the papillomavirus E6 interacting peptide E6ap},
5054 Uri = {<Go to ISI>://000183493500037},
5055 Volume = 100,
5056 Year = 2003}
5057
5058 @article{Denisov2003,
5059 Abstract = {We study the slow phase of thermally activated magnetic relaxation
5060 in finite two-dimensional ensembles of dipolar interacting ferromagnetic
5061 nanoparticles whose easy axes of magnetization are perpendicular
5062 to the distribution plane. We develop a method to numerically simulate
5063 the magnetic relaxation for the case that the smallest heights of
5064 the potential barriers between the equilibrium directions of the
5065 nanoparticle magnetic moments are much larger than the thermal energy.
5066 Within this framework, we analyze in detail the role that the correlations
5067 of the nanoparticle magnetic moments and the finite size of the
5068 nanoparticle ensemble play in magnetic relaxation.},
5069 Annote = {642XH Times Cited:11 Cited References Count:31},
5070 Author = {S. I. Denisov and T. V. Lyutyy and K. N. Trohidou},
5071 Issn = {1098-0121},
5072 Journal = {Physical Review B},
5073 Month = {Jan 1},
5074 Number = 1,
5075 Pages = {-},
5076 Title = {Magnetic relaxation in finite two-dimensional nanoparticle ensembles},
5077 Uri = {<Go to ISI>://000180830400056},
5078 Volume = 67,
5079 Year = 2003}
5080
5081 @article{Derreumaux1998,
5082 Abstract = {To explore the origin of the large-scale motion of triosephosphate
5083 isomerase's flexible loop (residues 166 to 176) at the active site,
5084 several simulation protocols are employed both for the free enzyme
5085 in vacuo and for the free enzyme with some solvent modeling: high-temperature
5086 Langevin dynamics simulations, sampling by a #dynamics##driver#
5087 approach, and potential-energy surface calculations. Our focus is
5088 on obtaining the energy barrier to the enzyme's motion and establishing
5089 the nature of the loop movement. Previous calculations did not determine
5090 this energy barrier and the effect of solvent on the barrier. High-temperature
5091 molecular dynamics simulations and crystallographic studies have
5092 suggested a rigid-body motion with two hinges located at both ends
5093 of the loop; Brownian dynamics simulations at room temperature pointed
5094 to a very flexible behavior. The present simulations and analyses
5095 reveal that although solute/solvent hydrogen bonds play a crucial
5096 role in lowering the energy along the pathway, there still remains
5097 a high activation barrier, This finding clearly indicates that,
5098 if the loop opens and closes in the absence of a substrate at standard
5099 conditions (e.g., room temperature, appropriate concentration of
5100 isomerase), the time scale for transition is not in the nanosecond
5101 but rather the microsecond range. Our results also indicate that
5102 in the context of spontaneous opening in the free enzyme, the motion
5103 is of rigid-body type and that the specific interaction between
5104 residues Ala(176) and Tyr(208) plays a crucial role in the loop
5105 opening/closing mechanism.},
5106 Annote = {Zl046 Times Cited:30 Cited References Count:29},
5107 Author = {P. Derreumaux and T. Schlick},
5108 Issn = {0006-3495},
5109 Journal = bj,
5110 Month = {Jan},
5111 Number = 1,
5112 Pages = {72-81},
5113 Title = {The loop opening/closing motion of the enzyme triosephosphate isomerase},
5114 Uri = {<Go to ISI>://000073393400009},
5115 Volume = 74,
5116 Year = 1998}
5117
5118 @article{Dullweber1997,
5119 Abstract = {Rigid body molecular models possess symplectic structure and time-reversal
5120 symmetry. Standard numerical integration methods destroy both properties,
5121 introducing nonphysical dynamical behavior such as numerically induced
5122 dissipative states and drift in the energy during long term simulations.
5123 This article describes the construction, implementation, and practical
5124 application of fast explicit symplectic-reversible integrators for
5125 multiple rigid body molecular simulations, These methods use a reduction
5126 to Euler equations for the free rigid body, together with a symplectic
5127 splitting technique. In every time step, the orientational dynamics
5128 of each rigid body is integrated by a sequence of planar rotations.
5129 Besides preserving the symplectic and reversible structures of the
5130 flow, this scheme accurately conserves the total angular momentum
5131 of a system of interacting rigid bodies. Excellent energy conservation
5132 fan be obtained relative to traditional methods, especially in long-time
5133 simulations. The method is implemented in a research code, ORIENT
5134 and compared with a quaternion/extrapolation scheme for the TIP4P
5135 model of water. Our experiments show that the symplectic-reversible
5136 scheme is far superior to the more traditional quaternion method.
5137 (C) 1997 American Institute of Physics.},
5138 Annote = {Ya587 Times Cited:35 Cited References Count:32},
5139 Author = {A. Dullweber and B. Leimkuhler and R. McLachlan},
5140 Issn = {0021-9606},
5141 Journal = jcp,
5142 Month = {Oct 15},
5143 Number = 15,
5144 Pages = {5840-5851},
5145 Title = {Symplectic splitting methods for rigid body molecular dynamics},
5146 Uri = {<Go to ISI>://A1997YA58700024},
5147 Volume = 107,
5148 Year = 1997}
5149
5150 @book{Gamma1994,
5151 Address = {London},
5152 Author = {E. Gamma, R. Helm, R. Johnson and J. Vlissides},
5153 Chapter = 7,
5154 Publisher = {Perason Education},
5155 Title = {Design Patterns: Elements of Reusable Object-Oriented Software},
5156 Year = 1994}
5157
5158 @article{Edwards2005,
5159 Abstract = {Using the Langevin dynamics technique, we have carried out simulations
5160 of a single-chain flexible diblock copolymer. The polymer consists
5161 of two blocks of equal length, one very poorly solvated and the
5162 other close to theta-conditions. We study what happens when such
5163 a polymer is stretched, for a range of different stretching speeds,
5164 and correlate our observations with features in the plot of force
5165 vs extension. We find that at slow speeds this force profile does
5166 not increase monotonically, in disagreement with earlier predictions,
5167 and that at high speeds there is a strong dependence on which end
5168 of the polymer is pulled, as well as a high level of hysteresis.},
5169 Annote = {992EC Times Cited:0 Cited References Count:13},
5170 Author = {S. A. Edwards and D. R. M. Williams},
5171 Issn = {0024-9297},
5172 Journal = {Macromolecules},
5173 Month = {Dec 13},
5174 Number = 25,
5175 Pages = {10590-10595},
5176 Title = {Stretching a single diblock copolymer in a selective solvent: Langevin dynamics simulations},
5177 Uri = {<Go to ISI>://000233866200035},
5178 Volume = 38,
5179 Year = 2005}
5180
5181 @article{Egberts1988,
5182 Annote = {Q0188 Times Cited:219 Cited References Count:43},
5183 Author = {E. Egberts and H. J. C. Berendsen},
5184 Issn = {0021-9606},
5185 Journal = jcp,
5186 Month = {Sep 15},
5187 Number = 6,
5188 Pages = {3718-3732},
5189 Title = {Molecular-Dynamics Simulation of a Smectic Liquid-Crystal with Atomic Detail},
5190 Uri = {<Go to ISI>://A1988Q018800036},
5191 Volume = 89,
5192 Year = 1988}
5193
5194 @article{Ermak1978,
5195 Annote = {Fp216 Times Cited:785 Cited References Count:42},
5196 Author = {D. L. Ermak and J. A. Mccammon},
5197 Issn = {0021-9606},
5198 Journal = jcp,
5199 Number = 4,
5200 Pages = {1352-1360},
5201 Title = {Brownian Dynamics with Hydrodynamic Interactions},
5202 Uri = {<Go to ISI>://A1978FP21600004},
5203 Volume = 69,
5204 Year = 1978}
5205
5206 @article{Evans1977,
5207 Annote = {Ds757 Times Cited:271 Cited References Count:18},
5208 Author = {D. J. Evans},
5209 Issn = {0026-8976},
5210 Journal = mp,
5211 Number = 2,
5212 Pages = {317-325},
5213 Title = {Representation of Orientation Space},
5214 Uri = {<Go to ISI>://A1977DS75700002},
5215 Volume = 34,
5216 Year = 1977}
5217
5218 @article{Fennell2004,
5219 Abstract = {The density maximum and temperature dependence of the self-diffusion
5220 constant were investigated for the soft sticky dipole (SSD) water
5221 model and two related reparametrizations of this single-point model.
5222 A combination of microcanonical and isobaric-isothermal molecular
5223 dynamics simulations was used to calculate these properties, both
5224 with and without the use of reaction field to handle long-range
5225 electrostatics. The isobaric-isothermal simulations of the melting
5226 of both ice-I-h and ice-I-c showed a density maximum near 260 K.
5227 In most cases, the use of the reaction field resulted in calculated
5228 densities which were significantly lower than experimental densities.
5229 Analysis of self-diffusion constants shows that the original SSD
5230 model captures the transport properties of experimental water very
5231 well in both the normal and supercooled liquid regimes. We also
5232 present our reparametrized versions of SSD for use both with the
5233 reaction field or without any long-range electrostatic corrections.
5234 These are called the SSD/RF and SSD/E models, respectively. These
5235 modified models were shown to maintain or improve upon the experimental
5236 agreement with the structural and transport properties that can
5237 be obtained with either the original SSD or the density-corrected
5238 version of the original model (SSD1). Additionally, a novel low-density
5239 ice structure is presented which appears to be the most stable ice
5240 structure for the entire SSD family. (C) 2004 American Institute
5241 of Physics.},
5242 Annote = {816YY Times Cited:5 Cited References Count:39},
5243 Author = {C. J. Fennell and J. D. Gezelter},
5244 Issn = {0021-9606},
5245 Journal = jcp,
5246 Month = {May 15},
5247 Number = 19,
5248 Pages = {9175-9184},
5249 Title = {On the structural and transport properties of the soft sticky dipole and related single-point water models},
5250 Uri = {<Go to ISI>://000221146400032},
5251 Volume = 120,
5252 Year = 2004}
5253
5254 @article{Fernandes2002,
5255 Abstract = {We have developed a Brownian dynamics simulation algorithm to generate
5256 Brownian trajectories of an isolated, rigid particle of arbitrary
5257 shape in the presence of electric fields or any other external agents.
5258 Starting from the generalized diffusion tensor, which can be calculated
5259 with the existing HYDRO software, the new program BROWNRIG (including
5260 a case-specific subprogram for the external agent) carries out a
5261 simulation that is analyzed later to extract the observable dynamic
5262 properties. We provide a variety of examples of utilization of this
5263 method, which serve as tests of its performance, and also illustrate
5264 its applicability. Examples include free diffusion, transport in
5265 an electric field, and diffusion in a restricting environment.},
5266 Annote = {633AD Times Cited:2 Cited References Count:43},
5267 Author = {M. X. Fernandes and {Garc\'{i}a de la Torre}, Jose},
5268 Issn = {0006-3495},
5269 Journal = bj,
5270 Month = {Dec},
5271 Number = 6,
5272 Pages = {3039-3048},
5273 Title = {Brownian dynamics simulation of rigid particles of arbitrary shape in external fields},
5274 Uri = {<Go to ISI>://000180256300012},
5275 Volume = 83,
5276 Year = 2002}
5277
5278 @book{Frenkel1996,
5279 Address = {New York},
5280 Author = {D. Frenkel and B. Smit},
5281 Publisher = {Academic Press},
5282 Title = {Understanding Molecular Simulation : From Algorithms to Applications},
5283 Year = 1996}
5284
5285 @article{Gay1981,
5286 Annote = {Lj347 Times Cited:482 Cited References Count:13},
5287 Author = {J. G. Gay and B. J. Berne},
5288 Issn = {0021-9606},
5289 Journal = jcp,
5290 Number = 6,
5291 Pages = {3316-3319},
5292 Title = {Modification of the Overlap Potential to Mimic a Linear Site-Site Potential},
5293 Uri = {<Go to ISI>://A1981LJ34700029},
5294 Volume = 74,
5295 Year = 1981}
5296
5297 @article{Gelin1999,
5298 Abstract = {To investigate the influence of inertial effects on the dynamics of
5299 an assembly of beads subjected to rigid constraints and placed in
5300 a buffer medium, a convenient method to introduce suitable generalized
5301 coordinates is presented. Without any restriction on the nature
5302 of the soft forces involved (both stochastic and deterministic),
5303 pertinent Langevin equations are derived. Provided that the Brownian
5304 forces are Gaussian and Markovian, the corresponding Fokker-Planck
5305 equation (FPE) is obtained in the complete phase space of generalized
5306 coordinates and momenta. The correct short time behavior for correlation
5307 functions (CFs) of generalized coordinates is established, and the
5308 diffusion equation with memory (DEM) is deduced from the FPE in
5309 the high friction Limit. The DEM is invoked to perform illustrative
5310 calculations in two dimensions of the orientational CFs for once
5311 broken nonrigid rods immobilized on a surface. These calculations
5312 reveal that the CFs under certain conditions exhibit an oscillatory
5313 behavior, which is irreproducible within the standard diffusion
5314 equation. Several methods are considered for the approximate solution
5315 of the DEM, and their application to three dimensional DEMs is discussed.},
5316 Annote = {257MM Times Cited:2 Cited References Count:82},
5317 Author = {M. F. Gelin},
5318 Issn = {1022-1344},
5319 Journal = {Macromolecular Theory and Simulations},
5320 Month = {Nov},
5321 Number = 6,
5322 Pages = {529-543},
5323 Title = {Inertial effects in the Brownian dynamics with rigid constraints},
5324 Uri = {<Go to ISI>://000083785700002},
5325 Volume = 8,
5326 Year = 1999}
5327
5328 @article{Goetz1998,
5329 Author = {R. Goetz and R. Lipowsky},
5330 Journal = jcp,
5331 Number = 17,
5332 Pages = 7397,
5333 Title = {Computer simulations of bilayer membranes: Self-assembly and interfacial tension},
5334 Volume = 108,
5335 Year = 1998}
5336
5337 @book{Goldstein2001,
5338 Address = {San Francisco},
5339 Author = {H. Goldstein and C. Poole and J. Safko},
5340 Edition = {3rd},
5341 Publisher = {Addison Wesley},
5342 Title = {Classical Mechanics},
5343 Year = 2001}
5344
5345 @article{Gray2003,
5346 Abstract = {Protein-protein docking algorithms provide a means to elucidate structural
5347 details for presently unknown complexes. Here, we present and evaluate
5348 a new method to predict protein-protein complexes from the coordinates
5349 of the unbound monomer components. The method employs a low-resolution,
5350 rigid-body, Monte Carlo search followed by simultaneous optimization
5351 of backbone displacement and side-chain conformations using Monte
5352 Carlo minimization. Up to 10(5) independent simulations are carried
5353 out, and the resulting #decoys# are ranked using an energy function
5354 dominated by van der Waals interactions, an implicit solvation model,
5355 and an orientation-dependent hydrogen bonding potential. Top-ranking
5356 decoys are clustered to select the final predictions. Small-perturbation
5357 studies reveal the formation of binding funnels in 42 of 54 cases
5358 using coordinates derived from the bound complexes and in 32 of
5359 54 cases using independently determined coordinates of one or both
5360 monomers. Experimental binding affinities correlate with the calculated
5361 score function and explain the predictive success or failure of
5362 many targets. Global searches using one or both unbound components
5363 predict at least 25% of the native residue-residue contacts in 28
5364 of the 32 cases where binding funnels exist. The results suggest
5365 that the method may soon be useful for generating models of biologically
5366 important complexes from the structures of the isolated components,
5367 but they also highlight the challenges that must be met to achieve
5368 consistent and accurate prediction of protein-protein interactions.
5369 (C) 2003 Elsevier Ltd. All rights reserved.},
5370 Annote = {704QL Times Cited:48 Cited References Count:60},
5371 Author = {J. J. Gray and S. Moughon and C. Wang and O. Schueler-Furman and B. Kuhlman and C. A. Rohl and D. Baker},
5372 Issn = {0022-2836},
5373 Journal = jmb,
5374 Month = {Aug 1},
5375 Number = 1,
5376 Pages = {281-299},
5377 Title = {Protein-protein docking with simultaneous optimization of rigid-body displacement and side-chain conformations},
5378 Uri = {<Go to ISI>://000184351300022},
5379 Volume = 331,
5380 Year = 2003}
5381
5382 @article{Greengard1994,
5383 Abstract = {Some of the recently developed fast summation methods that have arisen
5384 in scientific computing are described. These methods require an
5385 amount of work proportional to N or N log N to evaluate all pairwise
5386 interactions in an ensemble of N particles. Traditional methods,
5387 by contrast, require an amount of work proportional to N-2. AS a
5388 result, large-scale simulations can be carried out using only modest
5389 computer resources. In combination with supercomputers, it is possible
5390 to address questions that were previously out of reach. Problems
5391 from diffusion, gravitation, and wave propagation are considered.},
5392 Annote = {Pb499 Times Cited:99 Cited References Count:44},
5393 Author = {L. Greengard},
5394 Issn = {0036-8075},
5395 Journal = {Science},
5396 Month = {Aug 12},
5397 Number = 5174,
5398 Pages = {909-914},
5399 Title = {Fast Algorithms for Classical Physics},
5400 Uri = {<Go to ISI>://A1994PB49900031},
5401 Volume = 265,
5402 Year = 1994}
5403
5404 @article{Greengard1987,
5405 Annote = {L0498 Times Cited:899 Cited References Count:7},
5406 Author = {L. Greengard and V. Rokhlin},
5407 Issn = {0021-9991},
5408 Journal = jcop,
5409 Month = {Dec},
5410 Number = 2,
5411 Pages = {325-348},
5412 Title = {A Fast Algorithm for Particle Simulations},
5413 Uri = {<Go to ISI>://A1987L049800006},
5414 Volume = 73,
5415 Year = 1987}
5416
5417 @article{Hairer1997,
5418 Abstract = {Backward error analysis is a useful tool for the study of numerical
5419 approximations to ordinary differential equations. The numerical
5420 solution is formally interpreted as the exact solution of a perturbed
5421 differential equation, given as a formal and usually divergent series
5422 in powers of the step size. For a rigorous analysis, this series
5423 has to be truncated. In this article we study the influence of this
5424 truncation to the difference between the numerical solution and
5425 the exact solution of the perturbed differential equation. Results
5426 on the long-time behaviour of numerical solutions are obtained in
5427 this way. We present applications to the numerical phase portrait
5428 near hyperbolic equilibrium points, to asymptotically stable periodic
5429 orbits and Hopf bifurcation, and to energy conservation and approximation
5430 of invariant tori in Hamiltonian systems.},
5431 Annote = {Xj488 Times Cited:50 Cited References Count:19},
5432 Author = {E. Hairer and C. Lubich},
5433 Issn = {0029-599X},
5434 Journal = {Numerische Mathematik},
5435 Month = {Jun},
5436 Number = 4,
5437 Pages = {441-462},
5438 Title = {The life-span of backward error analysis for numerical integrators},
5439 Uri = {<Go to ISI>://A1997XJ48800002},
5440 Volume = 76,
5441 Year = 1997}
5442
5443 @article{Hao1993,
5444 Abstract = {A new procedure for studying the folding and unfolding of proteins,
5445 with an application to bovine pancreatic trypsin inhibitor (BPTI),
5446 is reported. The unfolding and refolding of the native structure
5447 of the protein are characterized by the dimensions of the protein,
5448 expressed in terms of the three principal radii of the structure
5449 considered as an ellipsoid. A dynamic equation, describing the variations
5450 of the principal radii on the unfolding path, and a numerical procedure
5451 to solve this equation are proposed. Expanded and distorted conformations
5452 are refolded to the native structure by a dimensional-constraint
5453 energy minimization procedure. A unique and reproducible unfolding
5454 pathway for an intermediate of BPTI lacking the [30,51] disulfide
5455 bond is obtained. The resulting unfolded conformations are extended;
5456 they contain near-native local structure, but their longest principal
5457 radii are more than 2.5 times greater than that of the native structure.
5458 The most interesting finding is that the majority of expanded conformations,
5459 generated under various conditions, can be refolded closely to the
5460 native structure, as measured by the correct overall chain fold,
5461 by the rms deviations from the native structure of only 1.9-3.1
5462 angstrom, and by the energy differences of about 10 kcal/mol from
5463 the native structure. Introduction of the [30,51] disulfide bond
5464 at this stage, followed by minimization, improves the closeness
5465 of the refolded structures to the native structure, reducing the
5466 rms deviations to 0.9-2.0 angstrom. The unique refolding of these
5467 expanded structures over such a large conformational space implies
5468 that the folding is strongly dictated by the interactions in the
5469 amino acid sequence of BPTI. The simulations indicate that, under
5470 conditions that favor a compact structure as mimicked by the volume
5471 constraints in our algorithm; the expanded conformations have a
5472 strong tendency to move toward the native structure; therefore,
5473 they probably would be favorable folding intermediates. The results
5474 presented here support a general model for protein folding, i.e.,
5475 progressive formation of partially folded structural units, followed
5476 by collapse to the compact native structure. The general applicability
5477 of the procedure is also discussed.},
5478 Annote = {Ly294 Times Cited:27 Cited References Count:57},
5479 Author = {M. H. Hao and M. R. Pincus and S. Rackovsky and H. A. Scheraga},
5480 Issn = {0006-2960},
5481 Journal = {Biochemistry},
5482 Month = {Sep 21},
5483 Number = 37,
5484 Pages = {9614-9631},
5485 Title = {Unfolding and Refolding of the Native Structure of Bovine Pancreatic Trypsin-Inhibitor Studied by Computer-Simulations},
5486 Uri = {<Go to ISI>://A1993LY29400014},
5487 Volume = 32,
5488 Year = 1993}
5489
5490 @article{Hinsen2000,
5491 Abstract = {The slow dynamics of proteins around its native folded state is usually
5492 described by diffusion in a strongly anharmonic potential. In this
5493 paper, we try to understand the form and origin of the anharmonicities,
5494 with the principal aim of gaining a better understanding of the
5495 principal motion types, but also in order to develop more efficient
5496 numerical methods for simulating neutron scattering spectra of large
5497 proteins. First, we decompose a molecular dynamics (MD) trajectory
5498 of 1.5 ns for a C-phycocyanin dimer surrounded by a layer of water
5499 into three contributions that we expect to be independent: the global
5500 motion of the residues, the rigid-body motion of the sidechains
5501 relative to the backbone, and the internal deformations of the sidechains.
5502 We show that they are indeed almost independent by verifying the
5503 factorization of the incoherent intermediate scattering function.
5504 Then, we show that the global residue motions, which include all
5505 large-scale backbone motions, can be reproduced by a simple harmonic
5506 model which contains two contributions: a short-time vibrational
5507 term, described by a standard normal mode calculation in a local
5508 minimum, and a long-time diffusive term, described by Brownian motion
5509 in an effective harmonic potential. The potential and the friction
5510 constants were fitted to the MD data. The major anharmonic contribution
5511 to the incoherent intermediate scattering function comes from the
5512 rigid-body diffusion of the sidechains. This model can be used to
5513 calculate scattering functions for large proteins and for long-time
5514 scales very efficiently, and thus provides a useful complement to
5515 MD simulations, which are best suited for detailed studies on smaller
5516 systems or for shorter time scales. (C) 2000 Elsevier Science B.V.
5517 All rights reserved.},
5518 Annote = {Sp. Iss. SI 368MT Times Cited:16 Cited References Count:31},
5519 Author = {K. Hinsen and A. J. Petrescu and S. Dellerue and M. C. Bellissent-Funel and G. R. Kneller},
5520 Issn = {0301-0104},
5521 Journal = {Chemical Physics},
5522 Month = {Nov 1},
5523 Number = {1-2},
5524 Pages = {25-37},
5525 Title = {Harmonicity in slow protein dynamics},
5526 Uri = {<Go to ISI>://000090121700003},
5527 Volume = 261,
5528 Year = 2000}
5529
5530 @article{Ho1992,
5531 Abstract = {Evidence has been found for the existence water at the protein-lipid
5532 hydrophobic interface ot the membrane proteins, gramicidin and apocytochrome
5533 C, using two related fluorescence spectroscopic approaches. The
5534 first approach exploited the fact that the presence of water in
5535 the excited state solvent cage of a fluorophore increases the rate
5536 of decay. For 1,6-diphenyl-1,3,5-hexatriene (DPH) and 1-palmitoyl-2-[[2-[4-(6-phenyl-trans-1,3,5-hexatrienyl)
5537 phenyl]ethyl]carbonyl]-3-sn-PC (DPH-PC), where the fluorophores
5538 are located in the hydrophobic core of the lipid bilayer, the introduction
5539 of gramicidin reduced the fluorescence lifetime, indicative of an
5540 increased presence of water in the bilayer. Since a high protein:lipid
5541 ratio was used, the fluorophores were forced to be adjacent to the
5542 protein hydrophobic surface, hence the presence of water in this
5543 region could be inferred. Cholesterol is known to reduce the water
5544 content of lipid bilayers and this effect was maintained at the
5545 protein-lipid interface with both gramicidin and apocytochrome C,
5546 again suggesting hydration in this region. The second approach was
5547 to use the fluorescence enhancement induced by exchanging deuterium
5548 oxide (D2O) for H2O. Both the fluorescence intensities of trimethylammonium-DPH,
5549 located in the lipid head group region, and of the gramicidin intrinsic
5550 tryptophans were greater in a D2O buffer compared with H2O, showing
5551 that the fluorophores were exposed to water in the bilayer at the
5552 protein-lipid interface. In the presence of cholesterol the fluorescence
5553 intensity ratio of D2O to H2O decreased, indicating a removal of
5554 water by the cholesterol, in keeping with the lifetime data. Altered
5555 hydration at the protein-lipid interface could affect conformation,
5556 thereby offering a new route by which membrane protein functioning
5557 may be modified.},
5558 Annote = {Ju251 Times Cited:55 Cited References Count:44},
5559 Author = {C. Ho and C. D. Stubbs},
5560 Issn = {0006-3495},
5561 Journal = bj,
5562 Month = {Oct},
5563 Number = 4,
5564 Pages = {897-902},
5565 Title = {Hydration at the Membrane Protein-Lipid Interface},
5566 Uri = {<Go to ISI>://A1992JU25100002},
5567 Volume = 63,
5568 Year = 1992}
5569
5570 @book{Hockney1981,
5571 Address = {New York},
5572 Author = {R.W. Hockney and J.W. Eastwood},
5573 Publisher = {McGraw-Hill},
5574 Title = {Computer Simulation Using Particles},
5575 Year = 1981}
5576
5577 @article{Hoover1985,
5578 Annote = {Acr30 Times Cited:1809 Cited References Count:11},
5579 Author = {W. G. Hoover},
5580 Issn = {1050-2947},
5581 Journal = {Physical Review A},
5582 Number = 3,
5583 Pages = {1695-1697},
5584 Title = {Canonical Dynamics - Equilibrium Phase-Space Distributions},
5585 Uri = {<Go to ISI>://A1985ACR3000056},
5586 Volume = 31,
5587 Year = 1985}
5588
5589 @article{Huh2004,
5590 Abstract = {Racemic fluids of chiral calamitic molecules are investigated with
5591 molecular dynamics simulations. In particular, the phase behavior
5592 as a function of density is examined for eight racemates. The relationship
5593 between chiral discrimination and orientational order in the phase
5594 is explored. We find that the transition from the isotropic phase
5595 to a liquid crystal phase is accompanied by an increase in chiral
5596 discrimination, as measured by differences in radial distributions.
5597 Among ordered phases, discrimination is largest for smectic phases
5598 with a significant preference for heterochiral contact within the
5599 layers. (C) 2004 American Institute of Physics.},
5600 Annote = {870FJ Times Cited:0 Cited References Count:63},
5601 Author = {Y. Huh and N. M. Cann},
5602 Issn = {0021-9606},
5603 Journal = jcp,
5604 Month = {Nov 22},
5605 Number = 20,
5606 Pages = {10299-10308},
5607 Title = {Discrimination in isotropic, nematic, and smectic phases of chiral calamitic molecules: A computer simulation study},
5608 Uri = {<Go to ISI>://000225042700059},
5609 Volume = 121,
5610 Year = 2004}
5611
5612 @article{Humphrey1996,
5613 Abstract = {VMD is a molecular graphics program designed for the display and analysis
5614 of molecular assemblies, in particular biopolymers such as proteins
5615 and nucleic acids. VMD can simultaneously display any number of
5616 structures using a wide variety of rendering styles and coloring
5617 methods. Molecules are displayed as one or more ''representations,''
5618 in which each representation embodies a particular rendering method
5619 and coloring scheme for a selected subset of atoms. The atoms displayed
5620 in each representation are chosen using an extensive atom selection
5621 syntax, which includes Boolean operators and regular expressions.
5622 VMD provides a complete graphical user interface for program control,
5623 as well as a text interface using the Tcl embeddable parser to allow
5624 for complex scripts with variable substitution, control loops, and
5625 function calls. Full session logging is supported, which produces
5626 a VMD command script for later playback. High-resolution raster
5627 images of displayed molecules may be produced by generating input
5628 scripts for use by a number of photorealistic image-rendering applications.
5629 VMD has also been expressly designed with the ability to animate
5630 molecular dynamics (MD) simulation trajectories, imported either
5631 from files or from a direct connection to a running MD simulation.
5632 VMD is the visualization component of MDScope, a set of tools for
5633 interactive problem solving in structural biology, which also includes
5634 the parallel MD program NAMD, and the MDCOMM software used to connect
5635 the visualization and simulation programs. VMD is written in C++,
5636 using an object-oriented design; the program, including source code
5637 and extensive documentation, is freely available via anonymous ftp
5638 and through the World Wide Web.},
5639 Annote = {Uh515 Times Cited:1418 Cited References Count:19},
5640 Author = {W. Humphrey and A. Dalke and K. Schulten},
5641 Issn = {0263-7855},
5642 Journal = {Journal of Molecular Graphics},
5643 Month = {Feb},
5644 Number = 1,
5645 Pages = {33-\&},
5646 Title = {VMD: Visual molecular dynamics},
5647 Uri = {<Go to ISI>://A1996UH51500005},
5648 Volume = 14,
5649 Year = 1996}
5650
5651 @article{Izaguirre2001,
5652 Abstract = {In this paper we show the possibility of using very mild stochastic
5653 damping to stabilize long time step integrators for Newtonian molecular
5654 dynamics. More specifically, stable and accurate integrations are
5655 obtained for damping coefficients that are only a few percent of
5656 the natural decay rate of processes of interest, such as the velocity
5657 autocorrelation function. Two new multiple time stepping integrators,
5658 Langevin Molly (LM) and Brunger-Brooks-Karplus-Molly (BBK-M), are
5659 introduced in this paper. Both use the mollified impulse method
5660 for the Newtonian term. LM uses a discretization of the Langevin
5661 equation that is exact for the constant force, and BBK-M uses the
5662 popular Brunger-Brooks-Karplus integrator (BBK). These integrators,
5663 along with an extrapolative method called LN, are evaluated across
5664 a wide range of damping coefficient values. When large damping coefficients
5665 are used, as one would for the implicit modeling of solvent molecules,
5666 the method LN is superior, with LM closely following. However, with
5667 mild damping of 0.2 ps(-1), LM produces the best results, allowing
5668 long time steps of 14 fs in simulations containing explicitly modeled
5669 flexible water. With BBK-M and the same damping coefficient, time
5670 steps of 12 fs are possible for the same system. Similar results
5671 are obtained for a solvated protein-DNA simulation of estrogen receptor
5672 ER with estrogen response element ERE. A parallel version of BBK-M
5673 runs nearly three times faster than the Verlet-I/r-RESPA (reversible
5674 reference system propagator algorithm) when using the largest stable
5675 time step on each one, and it also parallelizes well. The computation
5676 of diffusion coefficients for flexible water and ER/ERE shows that
5677 when mild damping of up to 0.2 ps-1 is used the dynamics are not
5678 significantly distorted. (C) 2001 American Institute of Physics.},
5679 Annote = {397CQ Times Cited:14 Cited References Count:36},
5680 Author = {J. A. Izaguirre and D. P. Catarello and J. M. Wozniak and R. D. Skeel},
5681 Issn = {0021-9606},
5682 Journal = jcp,
5683 Month = {Feb 1},
5684 Number = 5,
5685 Pages = {2090-2098},
5686 Title = {Langevin stabilization of molecular dynamics},
5687 Uri = {<Go to ISI>://000166676100020},
5688 Volume = 114,
5689 Year = 2001}
5690
5691 @article{Torre1977,
5692 Author = {{Garc\'{i}a de la Torre}, Jose and V.~A. Bloomfield},
5693 Journal = {Biopolymers},
5694 Pages = {1747-1763},
5695 Title = {Hydrodynamic properties of macromolecular complexes. I. Translation},
5696 Volume = 16,
5697 Year = 1977}
5698
5699 @article{Kale1999,
5700 Abstract = {Molecular dynamics programs simulate the behavior of biomolecular
5701 systems, leading to understanding of their functions. However, the
5702 computational complexity of such simulations is enormous. Parallel
5703 machines provide the potential to meet this computational challenge.
5704 To harness this potential, it is necessary to develop a scalable
5705 program. It is also necessary that the program be easily modified
5706 by application-domain programmers. The NAMD2 program presented in
5707 this paper seeks to provide these desirable features. It uses spatial
5708 decomposition combined with force decomposition to enhance scalability.
5709 It uses intelligent periodic load balancing, so as to maximally
5710 utilize the available compute power. It is modularly organized,
5711 and implemented using Charm++, a parallel C++ dialect, so as to
5712 enhance its modifiability. It uses a combination of numerical techniques
5713 and algorithms to ensure that energy drifts are minimized, ensuring
5714 accuracy in long running calculations. NAMD2 uses a portable run-time
5715 framework called Converse that also supports interoperability among
5716 multiple parallel paradigms. As a result, different components of
5717 applications can be written in the most appropriate parallel paradigms.
5718 NAMD2 runs on most parallel machines including workstation clusters
5719 and has yielded speedups in excess of 180 on 220 processors. This
5720 paper also describes the performance obtained on some benchmark
5721 applications. (C) 1999 Academic Press.},
5722 Annote = {194FM Times Cited:373 Cited References Count:51},
5723 Author = {L. Kale and R. Skeel and M. Bhandarkar and R. Brunner and A. Gursoy and N. Krawetz and J. Phillips and A. Shinozaki and K. Varadarajan and K. Schulten},
5724 Issn = {0021-9991},
5725 Journal = jcop,
5726 Month = {May 1},
5727 Number = 1,
5728 Pages = {283-312},
5729 Title = {NAMD2: Greater scalability for parallel molecular dynamics},
5730 Uri = {<Go to ISI>://000080181500013},
5731 Volume = 151,
5732 Year = 1999}
5733
5734 @article{Kane2000,
5735 Abstract = {The purpose of this work is twofold. First, we demonstrate analytically
5736 that the classical Newmark family as well as related integration
5737 algorithms are variational in the sense of the Veselov formulation
5738 of discrete mechanics. Such variational algorithms are well known
5739 to be symplectic and momentum preserving and to often have excellent
5740 global energy behaviour. This analytical result is verified through
5741 numerical examples and is believed to be one of the primary reasons
5742 that this class of algorithms performs so well. Second, we develop
5743 algorithms for mechanical systems with forcing, and in particular,
5744 for dissipative systems. In this case, we develop integrators that
5745 are based on a discretization of the Lagrange d'Alembert principle
5746 as well as on a variational formulation of dissipation. It is demonstrated
5747 that these types of structured integrators have good numerical behaviour
5748 in terms of obtaining the correct amounts by which the energy changes
5749 over the integration run. Copyright (C) 2000 John Wiley & Sons,
5750 Ltd.},
5751 Annote = {373CJ Times Cited:30 Cited References Count:41},
5752 Author = {C. Kane and J. E. Marsden and M. Ortiz and M. West},
5753 Issn = {0029-5981},
5754 Journal = {International Journal for Numerical Methods in Engineering},
5755 Month = {Dec 10},
5756 Number = 10,
5757 Pages = {1295-1325},
5758 Title = {Variational integrators and the Newmark algorithm for conservative and dissipative mechanical systems},
5759 Uri = {<Go to ISI>://000165270600004},
5760 Volume = 49,
5761 Year = 2000}
5762
5763 @article{Klimov1997,
5764 Abstract = {The viscosity (eta) dependence of the folding rates for four sequences
5765 (the native state of three sequences is a beta sheet, while the
5766 fourth forms an alpha helix) is calculated for off-lattice models
5767 of proteins. Assuming that the dynamics is given by the Langevin
5768 equation, we show that the folding rates increase linearly at low
5769 viscosities eta, decrease as 1/eta at large eta, and have a maximum
5770 at intermediate values. The Kramers' theory of barrier crossing
5771 provides a quantitative fit of the numerical results. By mapping
5772 the simulation results to real proteins we estimate that for optimized
5773 sequences the time scale for forming a four turn alpha-helix topology
5774 is about 500 ns, whereas for beta sheet it is about 10 mu s.},
5775 Annote = {Xk293 Times Cited:77 Cited References Count:17},
5776 Author = {D. K. Klimov and D. Thirumalai},
5777 Issn = {0031-9007},
5778 Journal = prl,
5779 Month = {Jul 14},
5780 Number = 2,
5781 Pages = {317-320},
5782 Title = {Viscosity dependence of the folding rates of proteins},
5783 Uri = {<Go to ISI>://A1997XK29300035},
5784 Volume = 79,
5785 Year = 1997}
5786
5787 @article{Kol1997,
5788 Abstract = {Rigid-body molecular dynamics simulations typically are performed
5789 in a quaternion representation. The nonseparable form of the Hamiltonian
5790 in quaternions prevents the use of a standard leapfrog (Verlet)
5791 integrator, so nonsymplectic Runge-Kutta, multistep, or extrapolation
5792 methods are generally used, This is unfortunate since symplectic
5793 methods like Verlet exhibit superior energy conservation in long-time
5794 integrations. In this article, we describe an alternative method,
5795 which we call RSHAKE (for rotation-SHAKE), in which the entire rotation
5796 matrix is evolved (using the scheme of McLachlan and Scovel [J.
5797 Nonlin. Sci, 16 233 (1995)]) in tandem with the particle positions.
5798 We employ a fast approximate Newton solver to preserve the orthogonality
5799 of the rotation matrix. We test our method on a system of soft-sphere
5800 dipoles and compare with quaternion evolution using a 4th-order
5801 predictor-corrector integrator, Although the short-time error of
5802 the quaternion algorithm is smaller for fixed time step than that
5803 for RSHAKE, the quaternion scheme exhibits an energy drift which
5804 is not observed in simulations with RSHAKE, hence a fixed energy
5805 tolerance can be achieved by using a larger time step, The superiority
5806 of RSHAKE increases with system size. (C) 1997 American Institute
5807 of Physics.},
5808 Annote = {Xq332 Times Cited:11 Cited References Count:18},
5809 Author = {A. Kol and B. B. Laird and B. J. Leimkuhler},
5810 Issn = {0021-9606},
5811 Journal = jcp,
5812 Month = {Aug 15},
5813 Number = 7,
5814 Pages = {2580-2588},
5815 Title = {A symplectic method for rigid-body molecular simulation},
5816 Uri = {<Go to ISI>://A1997XQ33200046},
5817 Volume = 107,
5818 Year = 1997}
5819
5820 @article{Lansac2001,
5821 Abstract = {Cyanobiphenyls (nCB's) represent a useful and intensively studied
5822 class of mesogens. Many of the peculiar properties of nCB's (e.g.,
5823 the occurence of the partial bilayer smectic-A(d) phase) are thought
5824 to be a manifestation of short-range antiparallel association of
5825 neighboring molecules, resulting from strong dipole-dipole interactions
5826 between cyano groups. To test and extend existing models of microscopic
5827 ordering in nCB's, we carry out large-scale atomistic simulation
5828 studies of the microscopic structure and dynamics of the Sm-A(d)
5829 phase of 4-octyl-4'-cyanobiphenyl (8CB). We compute a variety of
5830 thermodynamic, structural, and dynamical properties for this material,
5831 and make a detailed comparison of our results with experimental
5832 measurements in order to validate our molecular model. Semiquantitative
5833 agreement with experiment is found: the smectic layer spacing and
5834 mass density are well reproduced, translational diffusion constants
5835 are similar to experiment, but the orientational ordering of alkyl
5836 chains is overestimated. This simulation provides a detailed picture
5837 of molecular conformation, smectic layer structure, and intermolecular
5838 correlations in Sm-A(d) 8CB, and demonstrates that pronounced short-range
5839 antiparallel association of molecules arising from dipole-dipole
5840 interactions plays a dominant role in determining the molecular-scale
5841 structure of 8CB.},
5842 Annote = {Part 1 496QF Times Cited:10 Cited References Count:60},
5843 Author = {Y. Lansac and M. A. Glaser and N. A. Clark},
5844 Issn = {1063-651X},
5845 Journal = {Physical Review E},
5846 Month = {Nov},
5847 Number = 5,
5848 Pages = {-},
5849 Title = {Microscopic structure and dynamics of a partial bilayer smectic liquid crystal},
5850 Uri = {<Go to ISI>://000172406900063},
5851 Volume = 6405,
5852 Year = 2001}
5853
5854 @article{Lansac2003,
5855 Abstract = {Recently, a new class of smectic liquid crystal phases characterized
5856 by the spontaneous formation of macroscopic chiral domains from
5857 achiral bent-core molecules has been discovered. We have carried
5858 out Monte Carlo simulations of a minimal hard spherocylinder dimer
5859 model to investigate the role of excluded volume interactions in
5860 determining the phase behavior of bent-core materials and to probe
5861 the molecular origins of polar and chiral symmetry breaking. We
5862 present the phase diagram of hard spherocylinder dimers of length-diameter
5863 ratio of 5 as a function of pressure or density and dimer opening
5864 angle psi. With decreasing psi, a transition from a nonpolar to
5865 a polar smectic A phase is observed near psi=167degrees, and the
5866 nematic phase becomes thermodynamically unstable for psi<135degrees.
5867 Free energy calculations indicate that the antipolar smectic A (SmAP(A))
5868 phase is more stable than the polar smectic A phase (SmAP(F)). No
5869 chiral smectic or biaxial nematic phases were found.},
5870 Annote = {Part 1 646CM Times Cited:15 Cited References Count:38},
5871 Author = {Y. Lansac and P. K. Maiti and N. A. Clark and M. A. Glaser},
5872 Issn = {1063-651X},
5873 Journal = {Physical Review E},
5874 Month = {Jan},
5875 Number = 1,
5876 Pages = {-},
5877 Title = {Phase behavior of bent-core molecules},
5878 Uri = {<Go to ISI>://000181017300042},
5879 Volume = 67,
5880 Year = 2003}
5881
5882 @book{Leach2001,
5883 Address = {Harlow, England},
5884 Author = {A. Leach},
5885 Edition = {2nd},
5886 Publisher = {Pearson Educated Limited},
5887 Title = {Molecular Modeling: Principles and Applications},
5888 Year = 2001}
5889
5890 @article{Leimkuhler1999,
5891 Abstract = {Reversible and adaptive integration methods based on Kustaanheimo-Stiefel
5892 regularization and modified Sundman transformations are applied
5893 to simulate general perturbed Kepler motion and to compute classical
5894 trajectories of atomic systems (e.g. Rydberg atoms). The new family
5895 of reversible adaptive regularization methods also conserves angular
5896 momentum and exhibits superior energy conservation and numerical
5897 stability in long-time integrations. The schemes are appropriate
5898 for scattering, for astronomical calculations of escape time and
5899 long-term stability, and for classical and semiclassical studies
5900 of atomic dynamics. The components of an algorithm for trajectory
5901 calculations are described. Numerical experiments illustrate the
5902 effectiveness of the reversible approach.},
5903 Annote = {199EE Times Cited:11 Cited References Count:48},
5904 Author = {B. Leimkuhler},
5905 Issn = {1364-503X},
5906 Journal = {Philosophical Transactions of the Royal Society of London Series a-Mathematical Physical and Engineering Sciences},
5907 Month = {Apr 15},
5908 Number = 1754,
5909 Pages = {1101-1133},
5910 Title = {Reversible adaptive regularization: perturbed Kepler motion and classical atomic trajectories},
5911 Uri = {<Go to ISI>://000080466800007},
5912 Volume = 357,
5913 Year = 1999}
5914
5915 @book{Leimkuhler2004,
5916 Address = {Cambridge},
5917 Author = {B. Leimkuhler and S. Reich},
5918 Publisher = {Cambridge University Press},
5919 Title = {Simulating Hamiltonian Dynamics},
5920 Year = 2004}
5921
5922 @article{Levelut1981,
5923 Annote = {Ml751 Times Cited:96 Cited References Count:16},
5924 Author = {A. M. Levelut and R. J. Tarento and F. Hardouin and M. F. Achard and G. Sigaud},
5925 Issn = {1050-2947},
5926 Journal = {Physical Review A},
5927 Number = 4,
5928 Pages = {2180-2186},
5929 Title = {Number of Sa Phases},
5930 Uri = {<Go to ISI>://A1981ML75100057},
5931 Volume = 24,
5932 Year = 1981}
5933
5934 @article{Lieb1982,
5935 Annote = {Nu461 Times Cited:40 Cited References Count:28},
5936 Author = {W. R. Lieb and M. Kovalycsik and R. Mendelsohn},
5937 Issn = {0006-3002},
5938 Journal = {Biochimica Et Biophysica Acta},
5939 Number = 2,
5940 Pages = {388-398},
5941 Title = {Do Clinical-Levels of General-Anesthetics Affect Lipid Bilayers - Evidence from Raman-Scattering},
5942 Uri = {<Go to ISI>://A1982NU46100012},
5943 Volume = 688,
5944 Year = 1982}
5945
5946 @article{Link1997,
5947 Abstract = {A smectic liquid-crystal phase made from achiral molecules with bent
5948 cores was found to have fluid layers that exhibit two spontaneous
5949 symmetry-breaking instabilities: polar molecular orientational ordering
5950 about the layer normal and molecular tilt. These instabilities combine
5951 to form a chiral layer structure with a handedness that depends
5952 on the sign of the tilt. The bulk states are either antiferroelectric-racemic,
5953 with the layer polar direction and handedness alternating in sign
5954 from layer to layer, or antiferroelectric-chiral, which is of uniform
5955 layer handedness. Both states exhibit an electric field-induced
5956 transition from antiferroelectric to ferroelectric.},
5957 Annote = {Yl002 Times Cited:407 Cited References Count:25},
5958 Author = {D. R. Link and G. Natale and R. Shao and J. E. Maclennan and N. A. Clark and E. Korblova and D. M. Walba},
5959 Issn = {0036-8075},
5960 Journal = {Science},
5961 Month = {Dec 12},
5962 Number = 5345,
5963 Pages = {1924-1927},
5964 Title = {Spontaneous formation of macroscopic chiral domains in a fluid smectic phase of achiral molecules},
5965 Uri = {<Go to ISI>://A1997YL00200028},
5966 Volume = 278,
5967 Year = 1997}
5968
5969 @article{Liwo2005,
5970 Annote = {Suppl. 1 005MG Times Cited:0 Cited References Count:0},
5971 Author = {A. Liwo and M. Khalili and H. A. Scheraga},
5972 Issn = {1742-464X},
5973 Journal = {Febs Journal},
5974 Month = {Jul},
5975 Pages = {359-360},
5976 Title = {Ab initio simulations of protein folding pathways by molecular dynamics with the united-residue (UNRES) model of polypeptide chains},
5977 Uri = {<Go to ISI>://000234826102043},
5978 Volume = 272,
5979 Year = 2005}
5980
5981 @article{Luty1994,
5982 Abstract = {We compare the Particle-Particle Particle-Mesh (PPPM) and Ewald methods
5983 for calculating electrostatic interactions in periodic molecular
5984 systems. A brief comparison of the theories shows that the methods
5985 are very similar differing mainly in the technique which is used
5986 to perform the ''k-space'' or mesh calculation. Because the PPPM
5987 utilizes the highly efficient numerical Fast Fourier Transform (FFT)
5988 method it requires significantly less computational effort than
5989 the Ewald method and scale's almost linearly with system size.},
5990 Annote = {Qf464 Times Cited:50 Cited References Count:20},
5991 Author = {B. A. Luty and M. E. Davis and I. G. Tironi and W. F. Vangunsteren},
5992 Issn = {0892-7022},
5993 Journal = {Molecular Simulation},
5994 Number = 1,
5995 Pages = {11-20},
5996 Title = {A Comparison of Particle-Particle, Particle-Mesh and Ewald Methods for Calculating Electrostatic Interactions in Periodic Molecular-Systems},
5997 Uri = {<Go to ISI>://A1994QF46400002},
5998 Volume = 14,
5999 Year = 1994}
6000
6001 @book{Marion1990,
6002 Address = {New York},
6003 Author = {J.~B. Marion},
6004 Edition = {2rd},
6005 Publisher = {Academic Press},
6006 Title = {Classical Dynamics of Particles and Systems},
6007 Year = 1990}
6008
6009 @article{Marrink1994,
6010 Abstract = {To obtain insight in the process of water permeation through a lipid
6011 membrane, we performed molecular dynamics simulations on a phospholipid
6012 (DPPC)/water system with atomic detail. Since the actual process
6013 of permeation is too slow to be studied directly, we deduced the
6014 permeation rate indirectly via computation of the free energy and
6015 diffusion rate profiles of a water molecule across the bilayer.
6016 We conclude that the permeation of water through a lipid membrane
6017 cannot be described adequately by a simple homogeneous solubility-diffusion
6018 model. Both the excess free energy and the diffusion rate strongly
6019 depend on the position in the membrane, as a result from the inhomogeneous
6020 nature of the membrane. The calculated excess free energy profile
6021 has a shallow slope and a maximum height of 26 kJ/mol. The diffusion
6022 rate is highest in the middle of the membrane where the lipid density
6023 is low. In the interfacial region almost all water molecules are
6024 bound by the lipid headgroups, and the diffusion turns out to be
6025 1 order of magnitude smaller. The total transport process is essentially
6026 determined by the free energy barrier. The rate-limiting step is
6027 the permeation through the dense part of the lipid tails, where
6028 the resistance is highest. We found a permeation rate of 7(+/-3)
6029 x 10(-2) cm/s at 350 K, comparable to experimental values for DPPC
6030 membranes, if corrected for the temperature of the simulation. Taking
6031 the inhomogeneity of the membrane into account, we define a new
6032 ''four-region'' model which seems to be more realistic than the
6033 ''two-phase'' solubility-diffusion model.},
6034 Annote = {Ng219 Times Cited:187 Cited References Count:25},
6035 Author = {S. J. Marrink and H. J. C. Berendsen},
6036 Issn = {0022-3654},
6037 Journal = {Journal of Physical Chemistry},
6038 Month = {Apr 14},
6039 Number = 15,
6040 Pages = {4155-4168},
6041 Title = {Simulation of Water Transport through a Lipid-Membrane},
6042 Uri = {<Go to ISI>://A1994NG21900040},
6043 Volume = 98,
6044 Year = 1994}
6045
6046 @article{Marrink2004,
6047 Author = {S.~J. Marrink and A.~H. de~Vries and A.~E. Mark},
6048 Journal = {J. Phys. Chem. B},
6049 Pages = {750-760},
6050 Title = {Coarse Grained Model for Semiquantitative Lipid Simulations},
6051 Volume = 108,
6052 Year = 2004}
6053
6054 @article{Marsden1998,
6055 Abstract = {This paper presents a geometric-variational approach to continuous
6056 and discrete mechanics and field theories. Using multisymplectic
6057 geometry, we show that the existence of the fundamental geometric
6058 structures as well as their preservation along solutions can be
6059 obtained directly from the variational principle. In particular,
6060 we prove that a unique multisymplectic structure is obtained by
6061 taking the derivative of an action function, and use this structure
6062 to prove covariant generalizations of conservation of symplecticity
6063 and Noether's theorem. Natural discretization schemes for PDEs,
6064 which have these important preservation properties, then follow
6065 by choosing a discrete action functional. In the case of mechanics,
6066 we recover the variational symplectic integrators of Veselov type,
6067 while for PDEs we obtain covariant spacetime integrators which conserve
6068 the corresponding discrete multisymplectic form as well as the discrete
6069 momentum mappings corresponding to symmetries. We show that the
6070 usual notion of symplecticity along an infinite-dimensional space
6071 of fields can be naturally obtained by making a spacetime split.
6072 All of the aspects of our method are demonstrated with a nonlinear
6073 sine-Gordon equation, including computational results and a comparison
6074 with other discretization schemes.},
6075 Annote = {154RH Times Cited:88 Cited References Count:36},
6076 Author = {J. E. Marsden and G. W. Patrick and S. Shkoller},
6077 Issn = {0010-3616},
6078 Journal = {Communications in Mathematical Physics},
6079 Month = {Dec},
6080 Number = 2,
6081 Pages = {351-395},
6082 Title = {Multisymplectic geometry, variational integrators, and nonlinear PDEs},
6083 Uri = {<Go to ISI>://000077902200006},
6084 Volume = 199,
6085 Year = 1998}
6086
6087 @article{Matthey2004,
6088 Abstract = {PROTOMOL is a high-performance framework in C++ for rapid prototyping
6089 of novel algorithms for molecular dynamics and related applications.
6090 Its flexibility is achieved primarily through the use of inheritance
6091 and design patterns (object-oriented programming): Performance is
6092 obtained by using templates that enable generation of efficient
6093 code for sections critical to performance (generic programming).
6094 The framework encapsulates important optimizations that can be used
6095 by developers, such as parallelism in the force computation. Its
6096 design is based on domain analysis of numerical integrators for
6097 molecular dynamics (MD) and of fast solvers for the force computation,
6098 particularly due to electrostatic interactions. Several new and
6099 efficient algorithms are implemented in PROTOMOL. Finally, it is
6100 shown that PROTOMOL'S sequential performance is excellent when compared
6101 to a leading MD program, and that it scales well for moderate number
6102 of processors. Binaries and source codes for Windows, Linux, Solaris,
6103 IRIX, HP-UX, and AIX platforms are available under open source license
6104 at http://protomol.sourceforge.net.},
6105 Annote = {860EP Times Cited:2 Cited References Count:52},
6106 Author = {T. Matthey and T. Cickovski and S. Hampton and A. Ko and Q. Ma and M. Nyerges and T. Raeder and T. Slabach and J. A. Izaguirre},
6107 Issn = {0098-3500},
6108 Journal = {Acm Transactions on Mathematical Software},
6109 Month = {Sep},
6110 Number = 3,
6111 Pages = {237-265},
6112 Title = {ProtoMol, an object-oriented framework for prototyping novel algorithms for molecular dynamics},
6113 Uri = {<Go to ISI>://000224325600001},
6114 Volume = 30,
6115 Year = 2004}
6116
6117 @article{McLachlan1993,
6118 Author = {R.~I McLachlan},
6119 Journal = {prl},
6120 Pages = {3043-3046},
6121 Title = {Explicit Lie-Poisson integration and the Euler equations},
6122 Volume = 71,
6123 Year = 1993}
6124
6125 @article{McLachlan1998,
6126 Abstract = {We give a survey and some new examples of generating functions for
6127 systems with symplectic structure, systems with a first integral,
6128 systems that preserve volume, and systems with symmetries and/or
6129 time-reversing symmetries. Both ODEs and maps are treated, and we
6130 discuss how generating functions may be used in the structure-preserving
6131 numerical integration of ODEs with the above properties.},
6132 Annote = {Yt049 Times Cited:7 Cited References Count:26},
6133 Author = {R. I. McLachlan and G. R. W. Quispel},
6134 Issn = {0167-2789},
6135 Journal = {Physica D},
6136 Month = {Jan 15},
6137 Number = {1-2},
6138 Pages = {298-309},
6139 Title = {Generating functions for dynamical systems with symmetries, integrals, and differential invariants},
6140 Uri = {<Go to ISI>://000071558900021},
6141 Volume = 112,
6142 Year = 1998}
6143
6144 @article{McLachlan1998a,
6145 Abstract = {We consider properties of flows, the relationships between them, and
6146 whether numerical integrators can be made to preserve these properties.
6147 This is done in the context of automorphisms and antiautomorphisms
6148 of a certain group generated by maps associated to vector fields.
6149 This new framework unifies several known constructions. We also
6150 use the concept of #covariance# of a numerical method with respect
6151 to a group of coordinate transformations. The main application is
6152 to explore the relationship between spatial symmetries, reversing
6153 symmetries, and time symmetry of flows and numerical integrators.},
6154 Annote = {Zc449 Times Cited:14 Cited References Count:33},
6155 Author = {R. I. McLachlan and G. R. W. Quispel and G. S. Turner},
6156 Issn = {0036-1429},
6157 Journal = {Siam Journal on Numerical Analysis},
6158 Month = {Apr},
6159 Number = 2,
6160 Pages = {586-599},
6161 Title = {Numerical integrators that preserve symmetries and reversing symmetries},
6162 Uri = {<Go to ISI>://000072580500010},
6163 Volume = 35,
6164 Year = 1998}
6165
6166 @article{McLachlan2005,
6167 Abstract = {In this paper we revisit the Moser-Veselov description of the free
6168 rigid body in body coordinates, which, in the 3 x 3 case, can be
6169 implemented as an explicit, second-order, integrable approximation
6170 of the continuous solution. By backward error analysis, we study
6171 the modified vector field which is integrated exactly by the discrete
6172 algorithm. We deduce that the discrete Moser-Veselov (DMV) is well
6173 approximated to higher order by time reparametrizations of the continuous
6174 equations (modified vector field). We use the modified vector field
6175 to scale the initial data of the DMV to improve the order of the
6176 approximation and show the equivalence of the DMV and the RATTLE
6177 algorithm. Numerical integration with these preprocessed initial
6178 data is several orders of magnitude more accurate than the original
6179 DMV and RATTLE approach.},
6180 Annote = {911NS Times Cited:0 Cited References Count:14},
6181 Author = {R. I. McLachlan and A. Zanna},
6182 Issn = {1615-3375},
6183 Journal = {Foundations of Computational Mathematics},
6184 Month = {Feb},
6185 Number = 1,
6186 Pages = {87-123},
6187 Title = {The discrete Moser-Veselov algorithm for the free rigid body, revisited},
6188 Uri = {<Go to ISI>://000228011900003},
6189 Volume = 5,
6190 Year = 2005}
6191
6192 @article{Meineke2005,
6193 Abstract = {OOPSE is a new molecular dynamics simulation program that is capable
6194 of efficiently integrating equations of motion for atom types with
6195 orientational degrees of freedom (e.g. #sticky# atoms and point
6196 dipoles). Transition metals can also be simulated using the embedded
6197 atom method (EAM) potential included in the code. Parallel simulations
6198 are carried out using the force-based decomposition method. Simulations
6199 are specified using a very simple C-based meta-data language. A
6200 number of advanced integrators are included, and the basic integrator
6201 for orientational dynamics provides substantial improvements over
6202 older quaternion-based schemes. (C) 2004 Wiley Periodicals, Inc.},
6203 Annote = {891CF Times Cited:1 Cited References Count:56},
6204 Author = {M. A. Meineke and C. F. Vardeman and T. Lin and C. J. Fennell and J. D. Gezelter},
6205 Issn = {0192-8651},
6206 Journal = jcc,
6207 Month = {Feb},
6208 Number = 3,
6209 Pages = {252-271},
6210 Title = {OOPSE: An object-oriented parallel simulation engine for molecular dynamics},
6211 Uri = {<Go to ISI>://000226558200006},
6212 Volume = 26,
6213 Year = 2005}
6214
6215 @article{Melchionna1993,
6216 Abstract = {In this paper we write down equations of motion (following the approach
6217 pioneered by Hoover) for an exact isothermal-isobaric molecular
6218 dynamics simulation, and we extend them to multiple thermostating
6219 rates, to a shape-varying cell and to molecular systems, coherently
6220 with the previous 'extended system method'. An integration scheme
6221 is proposed together with a numerical illustration of the method.},
6222 Annote = {Kq355 Times Cited:172 Cited References Count:17},
6223 Author = {S. Melchionna and G. Ciccotti and B. L. Holian},
6224 Issn = {0026-8976},
6225 Journal = mp,
6226 Month = {Feb 20},
6227 Number = 3,
6228 Pages = {533-544},
6229 Title = {Hoover Npt Dynamics for Systems Varying in Shape and Size},
6230 Uri = {<Go to ISI>://A1993KQ35500002},
6231 Volume = 78,
6232 Year = 1993}
6233
6234 @article{Memmer2002,
6235 Abstract = {The phase behaviour of achiral banana-shaped molecules was studied
6236 by computer simulation. The banana-shaped molecules were described
6237 by model intermolecular interactions based on the Gay-Berne potential.
6238 The characteristic molecular structure was considered by joining
6239 two calamitic Gay-Berne particles through a bond to form a biaxial
6240 molecule of point symmetry group C-2v with a suitable bending angle.
6241 The dependence on temperature of systems of N=1024 rigid banana-shaped
6242 molecules with bending angle phi=140degrees has been studied by
6243 means of Monte Carlo simulations in the isobaric-isothermal ensemble
6244 (NpT). On cooling an isotropic system, two phase transitions characterized
6245 by phase transition enthalpy, entropy and relative volume change
6246 have been observed. For the first time by computer simulation of
6247 a many-particle system of banana-shaped molecules, at low temperature
6248 an untilted smectic phase showing a global phase biaxiality and
6249 a spontaneous local polarization in the layers, i.e. a local polar
6250 arrangement of the steric dipoles, with an antiferroelectric-like
6251 superstructure could be proven, a phase structure which recently
6252 has been discovered experimentally. Additionally, at intermediate
6253 temperature a nematic-like phase has been proved, whereas close
6254 to the transition to the smectic phase hints of a spontaneous achiral
6255 symmetry breaking have been determined. Here, in the absence of
6256 a layered structure a helical superstructure has been formed. All
6257 phases have been characterized by visual representations of selected
6258 configurations, scalar and pseudoscalar correlation functions, and
6259 order parameters.},
6260 Annote = {531HT Times Cited:12 Cited References Count:37},
6261 Author = {R. Memmer},
6262 Issn = {0267-8292},
6263 Journal = {Liquid Crystals},
6264 Month = {Apr},
6265 Number = 4,
6266 Pages = {483-496},
6267 Title = {Liquid crystal phases of achiral banana-shaped molecules: a computer simulation study},
6268 Uri = {<Go to ISI>://000174410500001},
6269 Volume = 29,
6270 Year = 2002}
6271
6272 @article{Metropolis1949,
6273 Author = {N. Metropolis and S. Ulam},
6274 Journal = {J. Am. Stat. Ass.},
6275 Pages = {335-341},
6276 Title = {The $\mbox{Monte Carlo}$ Method},
6277 Volume = 44,
6278 Year = 1949}
6279
6280 @article{Mielke2004,
6281 Abstract = {The torque generated by RNA polymerase as it tracks along double-stranded
6282 DNA can potentially induce long-range structural deformations integral
6283 to mechanisms of biological significance in both prokaryotes and
6284 eukaryotes. In this paper, we introduce a dynamic computer model
6285 for investigating this phenomenon. Duplex DNA is represented as
6286 a chain of hydrodynamic beads interacting through potentials of
6287 linearly elastic stretching, bending, and twisting, as well as excluded
6288 volume. The chain, linear when relaxed, is looped to form two open
6289 but topologically constrained subdomains. This permits the dynamic
6290 introduction of torsional stress via a centrally applied torque.
6291 We simulate by Brownian dynamics the 100 mus response of a 477-base
6292 pair B-DNA template to the localized torque generated by the prokaryotic
6293 transcription ensemble. Following a sharp rise at early times, the
6294 distributed twist assumes a nearly constant value in both subdomains,
6295 and a succession of supercoiling deformations occurs as superhelical
6296 stress is increasingly partitioned to writhe. The magnitude of writhe
6297 surpasses that of twist before also leveling off when the structure
6298 reaches mechanical equilibrium with the torsional load. Superhelicity
6299 is simultaneously right handed in one subdomain and left handed
6300 in the other, as predicted by the #transcription-induced##twin-supercoiled-domain#
6301 model [L. F. Liu and J. C. Wang, Proc. Natl. Acad. Sci. U.S.A. 84,
6302 7024 (1987)]. The properties of the chain at the onset of writhing
6303 agree well with predictions from theory, and the generated stress
6304 is ample for driving secondary structural transitions in physiological
6305 DNA. (C) 2004 American Institute of Physics.},
6306 Annote = {861ZF Times Cited:3 Cited References Count:34},
6307 Author = {S. P. Mielke and W. H. Fink and V. V. Krishnan and N. Gronbech-Jensen and C. J. Benham},
6308 Issn = {0021-9606},
6309 Journal = jcp,
6310 Month = {Oct 22},
6311 Number = 16,
6312 Pages = {8104-8112},
6313 Title = {Transcription-driven twin supercoiling of a DNA loop: A Brownian dynamics study},
6314 Uri = {<Go to ISI>://000224456500064},
6315 Volume = 121,
6316 Year = 2004}
6317
6318 @article{Naess2001,
6319 Abstract = {The three Eulerian angles constitute the classical choice of generalized
6320 coordinates used to describe the three degrees of rotational freedom
6321 of a rigid body, but it has long been known that this choice yields
6322 singular equations of motion. The latter is also true when Eulerian
6323 angles are used in Brownian dynamics analyses of the angular orientation
6324 of single rigid bodies and segmented polymer chains. Starting from
6325 kinetic theory we here show that by instead employing the three
6326 components of Cartesian rotation vectors as the generalized coordinates
6327 describing angular orientation, no singularity appears in the configuration
6328 space diffusion equation and the associated Brownian dynamics algorithm.
6329 The suitability of Cartesian rotation vectors in Brownian dynamics
6330 simulations of segmented polymer chains with spring-like or ball-socket
6331 joints is discussed. (C) 2001 Elsevier Science B.V. All rights reserved.},
6332 Annote = {433TA Times Cited:7 Cited References Count:19},
6333 Author = {S. N. Naess and H. M. Adland and A. Mikkelsen and A. Elgsaeter},
6334 Issn = {0378-4371},
6335 Journal = {Physica A},
6336 Month = {May 15},
6337 Number = {3-4},
6338 Pages = {323-339},
6339 Title = {Brownian dynamics simulation of rigid bodies and segmented polymer chains. Use of Cartesian rotation vectors as the generalized coordinates describing angular orientations},
6340 Uri = {<Go to ISI>://000168774800005},
6341 Volume = 294,
6342 Year = 2001}
6343
6344 @article{Niori1996,
6345 Abstract = {The synthesis of a banana-shaped molecule is reported and it is found
6346 that the smectic phase which it forms is biaxial with the molecules
6347 packed in the best,direction into a layer. Because of this characteristic
6348 packing, spontaneous polarization appears parallel to the layer
6349 and switches on reversal of an applied electric field. This is the
6350 first obvious example of ferroelectricity in an achiral smectic
6351 phase and is ascribed to the C-2v symmetry of the molecular packing.},
6352 Annote = {Ux855 Times Cited:447 Cited References Count:18},
6353 Author = {T. Niori and T. Sekine and J. Watanabe and T. Furukawa and H. Takezoe},
6354 Issn = {0959-9428},
6355 Journal = {Journal of Materials Chemistry},
6356 Month = {Jul},
6357 Number = 7,
6358 Pages = {1231-1233},
6359 Title = {Distinct ferroelectric smectic liquid crystals consisting of banana shaped achiral molecules},
6360 Uri = {<Go to ISI>://A1996UX85500025},
6361 Volume = 6,
6362 Year = 1996}
6363
6364 @article{Noguchi2002,
6365 Abstract = {We Studied the structural changes of bilayer vesicles induced by mechanical
6366 forces using a Brownian dynamics simulation. Two nanoparticles,
6367 which interact repulsively with amphiphilic molecules, are put inside
6368 a vesicle. The position of one nanoparticle is fixed, and the other
6369 is moved by a constant force as in optical-trapping experiments.
6370 First, the pulled vesicle stretches into a pear or tube shape. Then
6371 the inner monolayer in the tube-shaped region is deformed, and a
6372 cylindrical structure is formed between two vesicles. After stretching
6373 the cylindrical region, fission occurs near the moved vesicle. Soon
6374 after this the cylindrical region shrinks. The trapping force similar
6375 to 100 pN is needed to induce the formation of the cylindrical structure
6376 and fission.},
6377 Annote = {Part 1 568PX Times Cited:5 Cited References Count:39},
6378 Author = {H. Noguchi and M. Takasu},
6379 Issn = {1063-651X},
6380 Journal = {Physical Review E},
6381 Month = {may},
6382 Number = 5,
6383 Pages = {-},
6384 Title = {Structural changes of pulled vesicles: A Brownian dynamics simulation},
6385 Uri = {<Go to ISI>://000176552300084},
6386 Volume = 65,
6387 Year = 2002}
6388
6389 @article{Noguchi2001,
6390 Abstract = {We studied the fusion dynamics of vesicles using a Brownian dynamics
6391 simulation. Amphiphilic molecules spontaneously form vesicles with
6392 a bilayer structure. Two vesicles come into contact and form a stalk
6393 intermediate, in which a necklike structure only connects the outer
6394 monolayers, as predicted by the stalk hypothesis. We have found
6395 a new pathway of pore opening from stalks at high temperature: the
6396 elliptic stalk bends and contact between the ends of the arc-shaped
6397 stalk leads to pore opening. On the other hand, we have clarified
6398 that the pore-opening process at low temperature agrees with the
6399 modified stalk model: a pore is induced by contact between the inner
6400 monolayers inside the stalk. (C) 2001 American Institute of Physics.},
6401 Annote = {491UW Times Cited:48 Cited References Count:25},
6402 Author = {H. Noguchi and M. Takasu},
6403 Issn = {0021-9606},
6404 Journal = jcp,
6405 Month = {Nov 22},
6406 Number = 20,
6407 Pages = {9547-9551},
6408 Title = {Fusion pathways of vesicles: A Brownian dynamics simulation},
6409 Uri = {<Go to ISI>://000172129300049},
6410 Volume = 115,
6411 Year = 2001}
6412
6413 @book{Olver1986,
6414 Address = {New York},
6415 Author = {P.J. Olver},
6416 Publisher = {Springer},
6417 Title = {Applications of Lie groups to differential equatitons},
6418 Year = 1986}
6419
6420 @article{Omelyan1998,
6421 Abstract = {A revised version of the quaternion approach for numerical integration
6422 of the equations of motion for rigid polyatomic molecules is proposed.
6423 The modified approach is based on a formulation of the quaternion
6424 dynamics with constraints. This allows one to resolve the rigidity
6425 problem rigorously using constraint forces. It is shown that the
6426 procedure for preservation of molecular rigidity can be realized
6427 particularly simply within the Verlet algorithm in velocity form.
6428 We demonstrate that the method presented leads to an improved numerical
6429 stability with respect to the usual quaternion rescaling scheme
6430 and it is roughly as good as the cumbersome atomic-constraint technique.
6431 (C) 1998 American Institute of Physics.},
6432 Annote = {Yx279 Times Cited:12 Cited References Count:28},
6433 Author = {I. P. Omelyan},
6434 Issn = {0894-1866},
6435 Journal = {Computers in Physics},
6436 Month = {Jan-Feb},
6437 Number = 1,
6438 Pages = {97-103},
6439 Title = {On the numerical integration of motion for rigid polyatomics: The modified quaternion approach},
6440 Uri = {<Go to ISI>://000072024300025},
6441 Volume = 12,
6442 Year = 1998}
6443
6444 @article{Omelyan1998a,
6445 Abstract = {An algorithm for numerical integration of the rigid-body equations
6446 of motion is proposed. The algorithm uses the leapfrog scheme and
6447 the quantities involved are angular velocities and orientational
6448 variables that can be expressed in terms of either principal axes
6449 or quaternions. Due to specific features of the algorithm, orthonormality
6450 and unit norms of the orientational variables are integrals of motion,
6451 despite an approximate character of the produced trajectories. It
6452 is shown that the method presented appears to be the most efficient
6453 among all such algorithms known.},
6454 Annote = {101XL Times Cited:8 Cited References Count:22},
6455 Author = {I. P. Omelyan},
6456 Issn = {1063-651X},
6457 Journal = {Physical Review E},
6458 Month = {Jul},
6459 Number = 1,
6460 Pages = {1169-1172},
6461 Title = {Algorithm for numerical integration of the rigid-body equations of motion},
6462 Uri = {<Go to ISI>://000074893400151},
6463 Volume = 58,
6464 Year = 1998}
6465
6466 @article{Owren1992,
6467 Abstract = {Continuous, explicit Runge-Kutta methods with the minimal number of
6468 stages are considered. These methods are continuously differentiable
6469 if and only if one of the stages is the FSAL evaluation. A characterization
6470 of a subclass of these methods is developed for orders 3, 4, and
6471 5. It is shown how the free parameters of these methods can be used
6472 either to minimize the continuous truncation error coefficients
6473 or to maximize the stability region. As a representative for these
6474 methods the fifth-order method with minimized error coefficients
6475 is chosen, supplied with an error estimation method, and analysed
6476 by using the DETEST software. The results are compared with a similar
6477 implementation of the Dormand-Prince 5(4) pair with interpolant,
6478 showing a significant advantage in the new method for the chosen
6479 problems.},
6480 Annote = {Ju936 Times Cited:25 Cited References Count:20},
6481 Author = {B. Owren and M. Zennaro},
6482 Issn = {0196-5204},
6483 Journal = {Siam Journal on Scientific and Statistical Computing},
6484 Month = {Nov},
6485 Number = 6,
6486 Pages = {1488-1501},
6487 Title = {Derivation of Efficient, Continuous, Explicit Runge-Kutta Methods},
6488 Uri = {<Go to ISI>://A1992JU93600013},
6489 Volume = 13,
6490 Year = 1992}
6491
6492 @article{Palacios1998,
6493 Abstract = {The stochastic Landau-Lifshitz-Gilbert equation of motion for a classical
6494 magnetic moment is numerically solved (properly observing the customary
6495 interpretation of it as a Stratonovich stochastic differential equation),
6496 in order to study the dynamics of magnetic nanoparticles. The corresponding
6497 Langevin-dynamics approach allows for the study of the fluctuating
6498 trajectories of individual magnetic moments, where we have encountered
6499 remarkable phenomena in the overbarrier rotation process, such as
6500 crossing-back or multiple crossing of the potential barrier, rooted
6501 in the gyromagnetic nature of the system. Concerning averaged quantities,
6502 we study the linear dynamic response of the archetypal ensemble
6503 of noninteracting classical magnetic moments with axially symmetric
6504 magnetic anisotropy. The results are compared with different analytical
6505 expressions used to model the relaxation of nanoparticle ensembles,
6506 assessing their accuracy. It has been found that, among a number
6507 of heuristic expressions for the linear dynamic susceptibility,
6508 only the simple formula proposed by Shliomis and Stepanov matches
6509 the coarse features of the susceptibility reasonably. By comparing
6510 the numerical results with the asymptotic formula of Storonkin {Sov.
6511 Phys. Crystallogr. 30, 489 (1985) [Kristallografiya 30, 841 (1985)]},
6512 the effects of the intra-potential-well relaxation modes on the
6513 low-temperature longitudinal dynamic response have been assessed,
6514 showing their relatively small reflection in the susceptibility
6515 curves but their dramatic influence on the phase shifts. Comparison
6516 of the numerical results with the exact zero-damping expression
6517 for the transverse susceptibility by Garanin, Ishchenko, and Panina
6518 {Theor. Math. Phys. (USSR) 82, 169 (1990) [Teor. Mat. Fit. 82, 242
6519 (1990)]}, reveals a sizable contribution of the spread of the precession
6520 frequencies of the magnetic moment in the anisotropy field to the
6521 dynamic response at intermediate-to-high temperatures. [S0163-1829
6522 (98)00446-9].},
6523 Annote = {146XW Times Cited:66 Cited References Count:45},
6524 Author = {J. L. Garcia-Palacios and F. J. Lazaro},
6525 Issn = {0163-1829},
6526 Journal = {Physical Review B},
6527 Month = {Dec 1},
6528 Number = 22,
6529 Pages = {14937-14958},
6530 Title = {Langevin-dynamics study of the dynamical properties of small magnetic particles},
6531 Uri = {<Go to ISI>://000077460000052},
6532 Volume = 58,
6533 Year = 1998}
6534
6535 @article{Parr1995,
6536 Abstract = {Despite the parsing power of LR/LALR algorithms, e.g. YACC, programmers
6537 often choose to write recursive-descent parsers by hand to obtain
6538 increased flexibility, better error handling, and ease of debugging.
6539 We introduce ANTLR, a public-domain parser generator that combines
6540 the flexibility of hand-coded parsing with the convenience of a
6541 parser generator, which is a component of PCCTS. ANTLR has many
6542 features that make it easier to use than other language tools. Most
6543 important, ANTLR provides predicates which let the programmer systematically
6544 direct the parse via arbitrary expressions using semantic and syntactic
6545 context; in practice, the use of predicates eliminates the need
6546 to hand-tweak the ANTLR output, even for difficult parsing problems.
6547 ANTLR also integrates the description of lexical and syntactic analysis,
6548 accepts LL(k) grammars for k > 1 with extended BNF notation, and
6549 can automatically generate abstract syntax trees. ANTLR is widely
6550 used, with over 1000 registered industrial and academic users in
6551 37 countries. It has been ported to many popular systems such as
6552 the PC, Macintosh, and a variety of UNIX platforms; a commercial
6553 C++ front-end has been developed as a result of one of our industrial
6554 collaborations.},
6555 Annote = {Rk104 Times Cited:19 Cited References Count:10},
6556 Author = {T. J. Parr and R. W. Quong},
6557 Issn = {0038-0644},
6558 Journal = {Software-Practice \& Experience},
6559 Month = {Jul},
6560 Number = 7,
6561 Pages = {789-810},
6562 Title = {Antlr - a Predicated-Ll(K) Parser Generator},
6563 Uri = {<Go to ISI>://A1995RK10400004},
6564 Volume = 25,
6565 Year = 1995}
6566
6567 @article{Pastor1988,
6568 Annote = {T1302 Times Cited:61 Cited References Count:26},
6569 Author = {R. W. Pastor and B. R. Brooks and A. Szabo},
6570 Issn = {0026-8976},
6571 Journal = mp,
6572 Month = {Dec 20},
6573 Number = 6,
6574 Pages = {1409-1419},
6575 Title = {An Analysis of the Accuracy of Langevin and Molecular-Dynamics Algorithms},
6576 Uri = {<Go to ISI>://A1988T130200011},
6577 Volume = 65,
6578 Year = 1988}
6579
6580 @article{Pelzl1999,
6581 Annote = {220RC Times Cited:313 Cited References Count:49},
6582 Author = {G. Pelzl and S. Diele and W. Weissflog},
6583 Issn = {0935-9648},
6584 Journal = {Advanced Materials},
6585 Month = {Jul 5},
6586 Number = 9,
6587 Pages = {707-724},
6588 Title = {Banana-shaped compounds - A new field of liquid crystals},
6589 Uri = {<Go to ISI>://000081680400007},
6590 Volume = 11,
6591 Year = 1999}
6592
6593 @article{Perram1985,
6594 Annote = {Akb93 Times Cited:71 Cited References Count:12},
6595 Author = {J. W. Perram and M. S. Wertheim},
6596 Issn = {0021-9991},
6597 Journal = jcop,
6598 Number = 3,
6599 Pages = {409-416},
6600 Title = {Statistical-Mechanics of Hard Ellipsoids .1. Overlap Algorithm and the Contact Function},
6601 Uri = {<Go to ISI>://A1985AKB9300008},
6602 Volume = 58,
6603 Year = 1985}
6604
6605 @article{Rotne1969,
6606 Author = {F. Perrin},
6607 Journal = {J. Chem. Phys.},
6608 Pages = {4831-4837},
6609 Title = {Variational treatment of hydrodynamic interaction in polymers},
6610 Volume = 50,
6611 Year = 1969}
6612
6613 @article{Perrin1936,
6614 Author = {F. Perrin},
6615 Journal = {J. Phys. Radium},
6616 Pages = {1-11},
6617 Title = {Mouvement brownien d'un ellipsoid(II). Rotation libre et depolarisation des fluorescences. Translation et diffusion de moleculese ellipsoidales},
6618 Volume = 7,
6619 Year = 1936}
6620
6621 @article{Perrin1934,
6622 Author = {F. Perrin},
6623 Journal = {J. Phys. Radium},
6624 Pages = {497-511},
6625 Title = {Mouvement brownien d'un ellipsoid(I). Dispersion dielectrique pour des molecules ellipsoidales},
6626 Volume = 5,
6627 Year = 1934}
6628
6629 @article{Petrache2000,
6630 Author = {H.~I. Petrache and S.~W. Dodd and M.~F. Brown},
6631 Journal = bj,
6632 Pages = {3172-3192},
6633 Title = {Area per Lipid and Acyl Length Distributions in Fluid Phosphatidylcholines Determined by $^2\text{H}$ {\sc nmr} Spectroscopy},
6634 Volume = 79,
6635 Year = 2000}
6636
6637 @article{Petrache1998,
6638 Abstract = {X-ray diffraction data taken at high instrumental resolution were
6639 obtained for EPC and DMPC under various osmotic pressures, primarily
6640 at T = 30 degrees C. The headgroup thickness D-HH was obtained from
6641 relative electron density profiles. By using volumetric results
6642 and by comparing to gel phase DPPC we obtain areas A(EPC)(F) = 69.4
6643 +/- 1.1 Angstrom(2) and A(DMPC)(F) = 59.7 +/- 0.2 Angstrom(2). The
6644 analysis also gives estimates for the areal compressibility K-A.
6645 The A(F) results lead to other structural results regarding membrane
6646 thickness and associated waters. Using the recently determined absolute
6647 electrons density profile of DPPC, the AF results also lead to absolute
6648 electron density profiles and absolute continuous transforms \F(q)\
6649 for EPC and DMPC, Limited measurements of temperature dependence
6650 show directly that fluctuations increase with increasing temperature
6651 and that a small decrease in bending modulus K-c accounts for the
6652 increased water spacing reported by Simon et al. (1995) Biophys.
6653 J. 69, 1473-1483. (C) 1998 Elsevier Science Ireland Ltd. All rights
6654 reserved.},
6655 Annote = {130AT Times Cited:98 Cited References Count:39},
6656 Author = {H. I. Petrache and S. Tristram-Nagle and J. F. Nagle},
6657 Issn = {0009-3084},
6658 Journal = {Chemistry and Physics of Lipids},
6659 Month = {Sep},
6660 Number = 1,
6661 Pages = {83-94},
6662 Title = {Fluid phase structure of EPC and DMPC bilayers},
6663 Uri = {<Go to ISI>://000076497600007},
6664 Volume = 95,
6665 Year = 1998}
6666
6667 @article{Powles1973,
6668 Author = {J.~G. Powles},
6669 Journal = {Advan. Phys.},
6670 Pages = {1-56},
6671 Title = {A general ellipsoid can not always serve as a modle for the rotational diffusion properties of arbitrary shaped rigid molecules},
6672 Volume = 22,
6673 Year = 1973}
6674
6675 @article{Recio2004,
6676 Abstract = {Protein recognition is one of the most challenging and intriguing
6677 problems in structural biology. Despite all the available structural,
6678 sequence and biophysical information about protein-protein complexes,
6679 the physico-chemical patterns, if any, that make a protein surface
6680 likely to be involved in protein-protein interactions, remain elusive.
6681 Here, we apply protein docking simulations and analysis of the interaction
6682 energy landscapes to identify protein-protein interaction sites.
6683 The new protocol for global docking based on multi-start global
6684 energy optimization of an allatom model of the ligand, with detailed
6685 receptor potentials and atomic solvation parameters optimized in
6686 a training set of 24 complexes, explores the conformational space
6687 around the whole receptor without restrictions. The ensembles of
6688 the rigid-body docking solutions generated by the simulations were
6689 subsequently used to project the docking energy landscapes onto
6690 the protein surfaces. We found that highly populated low-energy
6691 regions consistently corresponded to actual binding sites. The procedure
6692 was validated on a test set of 21 known protein-protein complexes
6693 not used in the training set. As much as 81% of the predicted high-propensity
6694 patch residues were located correctly in the native interfaces.
6695 This approach can guide the design of mutations on the surfaces
6696 of proteins, provide geometrical details of a possible interaction,
6697 and help to annotate protein surfaces in structural proteomics.
6698 (C) 2003 Elsevier Ltd. All rights reserved.},
6699 Annote = {763GQ Times Cited:21 Cited References Count:59},
6700 Author = {J. Fernandez-Recio and M. Totrov and R. Abagyan},
6701 Issn = {0022-2836},
6702 Journal = jmb,
6703 Month = {Jan 16},
6704 Number = 3,
6705 Pages = {843-865},
6706 Title = {Identification of protein-protein interaction sites from docking energy landscapes},
6707 Uri = {<Go to ISI>://000188066900016},
6708 Volume = 335,
6709 Year = 2004}
6710
6711 @article{Reddy2006,
6712 Abstract = {An overview on the recent developments in the field of liquid crystalline
6713 bent-core molecules (so-called banana liquid crystals) is given.
6714 After some basic issues, dealing with general aspects of the systematisation
6715 of the mesophases, development of polar order and chirality in this
6716 class of LC systems and explaining some general structure-property
6717 relationships, we focus on fascinating new developments in this
6718 field, such as modulated, undulated and columnar phases, so-called
6719 B7 phases, phase biaxiality, ferroelectric and antiferroelectric
6720 polar order in smectic and columnar phases, amplification and switching
6721 of chirality and the spontaneous formation of superstructural and
6722 supramolecular chirality.},
6723 Annote = {021NS Times Cited:2 Cited References Count:316},
6724 Author = {R. A. Reddy and C. Tschierske},
6725 Issn = {0959-9428},
6726 Journal = {Journal of Materials Chemistry},
6727 Number = 10,
6728 Pages = {907-961},
6729 Title = {Bent-core liquid crystals: polar order, superstructural chirality and spontaneous desymmetrisation in soft matter systems},
6730 Uri = {<Go to ISI>://000235990500001},
6731 Volume = 16,
6732 Year = 2006}
6733
6734 @article{Reich1999,
6735 Abstract = {Backward error analysis has become an important tool for understanding
6736 the long time behavior of numerical integration methods. This is
6737 true in particular for the integration of Hamiltonian systems where
6738 backward error analysis can be used to show that a symplectic method
6739 will conserve energy over exponentially long periods of time. Such
6740 results are typically based on two aspects of backward error analysis:
6741 (i) It can be shown that the modified vector fields have some qualitative
6742 properties which they share with the given problem and (ii) an estimate
6743 is given for the difference between the best interpolating vector
6744 field and the numerical method. These aspects have been investigated
6745 recently, for example, by Benettin and Giorgilli in [J. Statist.
6746 Phys., 74 (1994), pp. 1117-1143], by Hairer in [Ann. Numer. Math.,
6747 1 (1994), pp. 107-132], and by Hairer and Lubich in [Numer. Math.,
6748 76 (1997), pp. 441-462]. In this paper we aim at providing a unifying
6749 framework and a simplification of the existing results and corresponding
6750 proofs. Our approach to backward error analysis is based on a simple
6751 recursive definition of the modified vector fields that does not
6752 require explicit Taylor series expansion of the numerical method
6753 and the corresponding flow maps as in the above-cited works. As
6754 an application we discuss the long time integration of chaotic Hamiltonian
6755 systems and the approximation of time averages along numerically
6756 computed trajectories.},
6757 Annote = {237HV Times Cited:43 Cited References Count:41},
6758 Author = {S. Reich},
6759 Issn = {0036-1429},
6760 Journal = {Siam Journal on Numerical Analysis},
6761 Month = {Sep 8},
6762 Number = 5,
6763 Pages = {1549-1570},
6764 Title = {Backward error analysis for numerical integrators},
6765 Uri = {<Go to ISI>://000082650600010},
6766 Volume = 36,
6767 Year = 1999}
6768
6769 @article{Ros2005,
6770 Abstract = {The recent literature in the field of liquid crystals shows that banana-shaped
6771 mesogenic materials represent a bewitching and stimulating field
6772 of research that is interesting both academically and in terms of
6773 applications. Numerous topics are open to investigation in this
6774 area because of the rich phenomenology and new possibilities that
6775 these materials offer. The principal concepts in this area are reviewed
6776 along with recent results. In addition, new directions to stimulate
6777 further research activities are highlighted.},
6778 Annote = {990XA Times Cited:3 Cited References Count:72},
6779 Author = {M. B. Ros and J. L. Serrano and M. R. {de la Fuente} and C. L. Folcia},
6780 Issn = {0959-9428},
6781 Journal = {Journal of Materials Chemistry},
6782 Number = 48,
6783 Pages = {5093-5098},
6784 Title = {Banana-shaped liquid crystals: a new field to explore},
6785 Uri = {<Go to ISI>://000233775500001},
6786 Volume = 15,
6787 Year = 2005}
6788
6789 @article{Roux1991,
6790 Abstract = {The mobility of water, Na+. and K+ has been calculated inside a periodic
6791 poly-(L,D)-alanine beta-helix, a model for the interior of the gramicidin
6792 channel. Because of the different dynamical regimes for the three
6793 species (high barrier for Na+, low barrier for K+, almost free diffusion
6794 for water), different methods are used to calculate the mobilities.
6795 By use of activated dynamics and a potential of mean force determined
6796 previously (Roux, B.; Karplus, M. Biophys. J. 1991, 59, 961), the
6797 barrier crossing rate of Na+ ion is determined. The motion of Na+
6798 at the transition state is controlled by local interactions and
6799 collisions with the neighboring carbonyls and the two nearest water
6800 molecules. There are significant deviations from transition-state
6801 theory; the transmission coefficient is equal to 0.11. The water
6802 and K+ motions are found to be well described by a diffusive model;
6803 the motion of K+ appears to be controlled by the diffusion of water.
6804 The time-dependent friction functions of Na+ and K+ ions in the
6805 periodic beta-helix are calculated and analyzed by using a generalized
6806 Langevin equation approach. Both Na+ and K+ suffer many rapid collisions,
6807 and their dynamics is overdamped and noninertial. Thus, the selectivity
6808 sequence of ions in the beta-helix is not influenced strongly by
6809 their masses.},
6810 Annote = {Fr756 Times Cited:97 Cited References Count:65},
6811 Author = {B. Roux and M. Karplus},
6812 Issn = {0022-3654},
6813 Journal = {Journal of Physical Chemistry},
6814 Month = {Jun 13},
6815 Number = 12,
6816 Pages = {4856-4868},
6817 Title = {Ion-Transport in a Gramicidin-Like Channel - Dynamics and Mobility},
6818 Uri = {<Go to ISI>://A1991FR75600049},
6819 Volume = 95,
6820 Year = 1991}
6821
6822 @article{Roy2005,
6823 Abstract = {A vast majority of compounds with bent core or banana shaped molecules
6824 exhibit the phase sequence B-6-B-1-B-2 as the chain length is increased
6825 in a homologous series. The B-6 phase has an intercalated fluid
6826 lamellar structure with a layer spacing of half the molecular length.
6827 The B-1 phase has a two dimensionally periodic rectangular columnar
6828 structure. The B-2 phase has a monolayer fluid lamellar structure
6829 with molecules tilted with respect to the layer normal. Neglecting
6830 the tilt order of the molecules in the B-2 phase, we have developed
6831 a frustrated packing model to describe this phase sequence qualitatively.
6832 The model has some analogy with that of the frustrated smectics
6833 exhibited by highly polar rod like molecules.},
6834 Annote = {985FW Times Cited:0 Cited References Count:30},
6835 Author = {A. Roy and N. V. Madhusudana},
6836 Issn = {1292-8941},
6837 Journal = {European Physical Journal E},
6838 Month = {Nov},
6839 Number = 3,
6840 Pages = {253-258},
6841 Title = {A frustrated packing model for the B-6-B-1-SmAP(A) sequence of phases in banana shaped molecules},
6842 Uri = {<Go to ISI>://000233363300002},
6843 Volume = 18,
6844 Year = 2005}
6845
6846 @article{Ryckaert1977,
6847 Annote = {Cz253 Times Cited:3680 Cited References Count:7},
6848 Author = {J. P. Ryckaert and G. Ciccotti and H. J. C. Berendsen},
6849 Issn = {0021-9991},
6850 Journal = jcop,
6851 Number = 3,
6852 Pages = {327-341},
6853 Title = {Numerical-Integration of Cartesian Equations of Motion of a System with Constraints - Molecular-Dynamics of N-Alkanes},
6854 Uri = {<Go to ISI>://A1977CZ25300007},
6855 Volume = 23,
6856 Year = 1977}
6857
6858 @article{Sagui1999,
6859 Abstract = {Current computer simulations of biomolecules typically make use of
6860 classical molecular dynamics methods, as a very large number (tens
6861 to hundreds of thousands) of atoms are involved over timescales
6862 of many nanoseconds. The methodology for treating short-range bonded
6863 and van der Waals interactions has matured. However, long-range
6864 electrostatic interactions still represent a bottleneck in simulations.
6865 In this article, we introduce the basic issues for an accurate representation
6866 of the relevant electrostatic interactions. In spite of the huge
6867 computational time demanded by most biomolecular systems, it is
6868 no longer necessary to resort to uncontrolled approximations such
6869 as the use of cutoffs. In particular, we discuss the Ewald summation
6870 methods, the fast particle mesh methods, and the fast multipole
6871 methods. We also review recent efforts to understand the role of
6872 boundary conditions in systems with long-range interactions, and
6873 conclude with a short perspective on future trends.},
6874 Annote = {213KJ Times Cited:126 Cited References Count:73},
6875 Author = {C. Sagui and T. A. Darden},
6876 Issn = {1056-8700},
6877 Journal = {Annual Review of Biophysics and Biomolecular Structure},
6878 Pages = {155-179},
6879 Title = {Molecular dynamics simulations of biomolecules: Long-range electrostatic effects},
6880 Uri = {<Go to ISI>://000081271400008},
6881 Volume = 28,
6882 Year = 1999}
6883
6884 @article{Sandu1999,
6885 Abstract = {Numerical resonance artifacts have become recognized recently as a
6886 limiting factor to increasing the timestep in multiple-timestep
6887 (MTS) biomolecular dynamics simulations. At certain timesteps correlated
6888 to internal motions (e.g., 5 fs, around half the period of the fastest
6889 bond stretch, T-min), visible inaccuracies or instabilities can
6890 occur. Impulse-MTS schemes are vulnerable to these resonance errors
6891 since large energy pulses are introduced to the governing dynamics
6892 equations when the slow forces are evaluated. We recently showed
6893 that such resonance artifacts can be masked significantly by applying
6894 extrapolative splitting to stochastic dynamics. Theoretical and
6895 numerical analyses of force-splitting integrators based on the Verlet
6896 discretization are reported here for linear models to explain these
6897 observations and to suggest how to construct effective integrators
6898 for biomolecular dynamics that balance stability with accuracy.
6899 Analyses for Newtonian dynamics demonstrate the severe resonance
6900 patterns of the Impulse splitting, with this severity worsening
6901 with the outer timestep. Delta t: Constant Extrapolation is generally
6902 unstable, but the disturbances do not grow with Delta t. Thus. the
6903 stochastic extrapolative combination can counteract generic instabilities
6904 and largely alleviate resonances with a sufficiently strong Langevin
6905 heat-bath coupling (gamma), estimates for which are derived here
6906 based on the fastest and slowest motion periods. These resonance
6907 results generally hold for nonlinear test systems: a water tetramer
6908 and solvated protein. Proposed related approaches such as Extrapolation/Correction
6909 and Midpoint Extrapolation work better than Constant Extrapolation
6910 only for timesteps less than T-min/2. An effective extrapolative
6911 stochastic approach for biomolecules that balances long-timestep
6912 stability with good accuracy for the fast subsystem is then applied
6913 to a biomolecule using a three-class partitioning: the medium forces
6914 are treated by Midpoint Extrapolation via position Verlet, and the
6915 slow forces are incorporated by Constant Extrapolation. The resulting
6916 algorithm (LN) performs well on a solvated protein system in terms
6917 of thermodynamic properties and yields an order of magnitude speedup
6918 with respect to single-timestep Langevin trajectories. Computed
6919 spectral density functions also show how the Newtonian modes can
6920 be approximated by using a small gamma in the range Of 5-20 ps(-1).
6921 (C) 1999 Academic Press.},
6922 Annote = {194FM Times Cited:14 Cited References Count:32},
6923 Author = {A. Sandu and T. Schlick},
6924 Issn = {0021-9991},
6925 Journal = jcop,
6926 Month = {May 1},
6927 Number = 1,
6928 Pages = {74-113},
6929 Title = {Masking resonance artifacts in force-splitting methods for biomolecular simulations by extrapolative Langevin dynamics},
6930 Uri = {<Go to ISI>://000080181500004},
6931 Volume = 151,
6932 Year = 1999}
6933
6934 @article{Sasaki2004,
6935 Abstract = {Tris(2-aminoethyl) amine derivatives with appended urea and sulfonamide
6936 groups are shown to facilitate the translocation of fluorescent
6937 phospholipid probes and endogenous phosphatidylserine across vesicle
6938 and erythrocyte cell membranes. The synthetic translocases appear
6939 to operate by binding to the phospholipid head groups and forming
6940 lipophilic supramolecular complexes which diffuse through the non-polar
6941 interior of the bilayer membrane.},
6942 Annote = {760PX Times Cited:8 Cited References Count:25},
6943 Author = {Y. Sasaki and R. Shukla and B. D. Smith},
6944 Issn = {1477-0520},
6945 Journal = {Organic \& Biomolecular Chemistry},
6946 Number = 2,
6947 Pages = {214-219},
6948 Title = {Facilitated phosphatidylserine flip-flop across vesicle and cell membranes using urea-derived synthetic translocases},
6949 Uri = {<Go to ISI>://000187843800012},
6950 Volume = 2,
6951 Year = 2004}
6952
6953 @article{Satoh1996,
6954 Abstract = {The effects of dipole-dipole interaction on mesophase formation are
6955 investigated with a Monte Carlo simulation using the dipolar Gay-Berne
6956 potential. It is shown that the dipole moment at the end of a molecule
6957 causes a shift in the nematic-isotropic transition toward higher
6958 temperature and a spread of the temperature range of the nematic
6959 phase and that layer structures with various interdigitations are
6960 formed in the smectic phase.},
6961 Annote = {Uq975 Times Cited:32 Cited References Count:33},
6962 Author = {K. Satoh and S. Mita and S. Kondo},
6963 Issn = {0009-2614},
6964 Journal = {Chemical Physics Letters},
6965 Month = {Jun 7},
6966 Number = {1-3},
6967 Pages = {99-104},
6968 Title = {Monte Carlo simulations using the dipolar Gay-Berne model: Effect of terminal dipole moment on mesophase formation},
6969 Uri = {<Go to ISI>://A1996UQ97500017},
6970 Volume = 255,
6971 Year = 1996}
6972
6973 @article{Schaps1999,
6974 Annote = {163EC Times Cited:0 Cited References Count:0},
6975 Author = {G. L. Schaps},
6976 Issn = {1044-789X},
6977 Journal = {Dr Dobbs Journal},
6978 Month = {Mar},
6979 Number = 3,
6980 Pages = {84-+},
6981 Title = {Compiler construction with ANTLR and Java - Tools for building tools},
6982 Uri = {<Go to ISI>://000078389200023},
6983 Volume = 24,
6984 Year = 1999}
6985
6986 @article{Shen2002,
6987 Abstract = {Met-enkephalin is one of the smallest opiate peptides. Yet, its dynamical
6988 structure and receptor docking mechanism are still not well understood.
6989 The conformational dynamics of this neuron peptide in liquid water
6990 are studied here by using all-atom molecular dynamics (MID) and
6991 implicit water Langevin dynamics (LD) simulations with AMBER potential
6992 functions and the three-site transferable intermolecular potential
6993 (TIP3P) model for water. To achieve the same simulation length in
6994 physical time, the full MID simulations require 200 times as much
6995 CPU time as the implicit water LID simulations. The solvent hydrophobicity
6996 and dielectric behavior are treated in the implicit solvent LD simulations
6997 by using a macroscopic solvation potential, a single dielectric
6998 constant, and atomic friction coefficients computed using the accessible
6999 surface area method with the TIP3P model water viscosity as determined
7000 here from MID simulations for pure TIP3P water. Both the local and
7001 the global dynamics obtained from the implicit solvent LD simulations
7002 agree very well with those from the explicit solvent MD simulations.
7003 The simulations provide insights into the conformational restrictions
7004 that are associated with the bioactivity of the opiate peptide dermorphin
7005 for the delta-receptor.},
7006 Annote = {540MH Times Cited:36 Cited References Count:45},
7007 Author = {M. Y. Shen and K. F. Freed},
7008 Issn = {0006-3495},
7009 Journal = bj,
7010 Month = {Apr},
7011 Number = 4,
7012 Pages = {1791-1808},
7013 Title = {Long time dynamics of met-enkephalin: Comparison of explicit and implicit solvent models},
7014 Uri = {<Go to ISI>://000174932400010},
7015 Volume = 82,
7016 Year = 2002}
7017
7018 @article{Shillcock2005,
7019 Annote = {901QJ Times Cited:9 Cited References Count:23},
7020 Author = {J. C. Shillcock and R. Lipowsky},
7021 Issn = {1476-1122},
7022 Journal = {Nature Materials},
7023 Month = {Mar},
7024 Number = 3,
7025 Pages = {225-228},
7026 Title = {Tension-induced fusion of bilayer membranes and vesicles},
7027 Uri = {<Go to ISI>://000227296700019},
7028 Volume = 4,
7029 Year = 2005}
7030
7031 @article{Shimada1993,
7032 Abstract = {To make improved treatments of electrostatic interactions in biomacromolecular
7033 simulations, two possibilities are considered. The first is the
7034 famous particle-particle and particle-mesh (PPPM) method developed
7035 by Hockney and Eastwood, and the second is a new one developed here
7036 in their spirit but by the use of the multipole expansion technique
7037 suggested by Ladd. It is then numerically found that the new PPPM
7038 method gives more accurate results for a two-particle system at
7039 small separation of particles. Preliminary numerical examination
7040 of the various computational methods for a single configuration
7041 of a model BPTI-water system containing about 24,000 particles indicates
7042 that both of the PPPM methods give far more accurate values with
7043 reasonable computational cost than do the conventional truncation
7044 methods. It is concluded the two PPPM methods are nearly comparable
7045 in overall performance for the many-particle systems, although the
7046 first method has the drawback that the accuracy in the total electrostatic
7047 energy is not high for configurations of charged particles randomly
7048 generated.},
7049 Annote = {Lh164 Times Cited:27 Cited References Count:47},
7050 Author = {J. Shimada and H. Kaneko and T. Takada},
7051 Issn = {0192-8651},
7052 Journal = jcc,
7053 Month = {Jul},
7054 Number = 7,
7055 Pages = {867-878},
7056 Title = {Efficient Calculations of Coulombic Interactions in Biomolecular Simulations with Periodic Boundary-Conditions},
7057 Uri = {<Go to ISI>://A1993LH16400011},
7058 Volume = 14,
7059 Year = 1993}
7060
7061 @article{Skeel2002,
7062 Abstract = {The best simple method for Newtonian molecular dynamics is indisputably
7063 the leapfrog Stormer-Verlet method. The appropriate generalization
7064 to simple Langevin dynamics is unclear. An analysis is presented
7065 comparing an 'impulse method' (kick; fluctuate; kick), the 1982
7066 method of van Gunsteren and Berendsen, and the Brunger-Brooks-Karplus
7067 (BBK) method. It is shown how the impulse method and the van Gunsteren-Berendsen
7068 methods can be implemented as efficiently as the BBK method. Other
7069 considerations suggest that the impulse method is the best basic
7070 method for simple Langevin dynamics, with the van Gunsteren-Berendsen
7071 method a close contender.},
7072 Annote = {633RX Times Cited:8 Cited References Count:22},
7073 Author = {R. D. Skeel and J. A. Izaguirre},
7074 Issn = {0026-8976},
7075 Journal = mp,
7076 Month = {Dec 20},
7077 Number = 24,
7078 Pages = {3885-3891},
7079 Title = {An impulse integrator for Langevin dynamics},
7080 Uri = {<Go to ISI>://000180297200014},
7081 Volume = 100,
7082 Year = 2002}
7083
7084 @article{Skeel1997,
7085 Abstract = {The following integration methods for special second-order ordinary
7086 differential equations are studied: leapfrog, implicit midpoint,
7087 trapezoid, Stormer-Verlet, and Cowell-Numerov. We show that all
7088 are members, or equivalent to members, of a one-parameter family
7089 of schemes. Some methods have more than one common form, and we
7090 discuss a systematic enumeration of these forms. We also present
7091 a stability and accuracy analysis based on the idea of ''modified
7092 equations'' and a proof of symplecticness. It follows that Cowell-Numerov
7093 and ''LIM2'' (a method proposed by Zhang and Schlick) are symplectic.
7094 A different interpretation of the values used by these integrators
7095 leads to higher accuracy and better energy conservation. Hence,
7096 we suggest that the straightforward analysis of energy conservation
7097 is misleading.},
7098 Annote = {We981 Times Cited:30 Cited References Count:35},
7099 Author = {R. D. Skeel and G. H. Zhang and T. Schlick},
7100 Issn = {1064-8275},
7101 Journal = {Siam Journal on Scientific Computing},
7102 Month = {Jan},
7103 Number = 1,
7104 Pages = {203-222},
7105 Title = {A family of symplectic integrators: Stability, accuracy, and molecular dynamics applications},
7106 Uri = {<Go to ISI>://A1997WE98100012},
7107 Volume = 18,
7108 Year = 1997}
7109
7110 @article{Tao2005,
7111 Abstract = {Recently a microscopic theory for the dynamics of suspensions of long
7112 thin rigid rods was presented, confirming and expanding the well-known
7113 theory by Doi and Edwards [The Theory of Polymer Dynamics (Clarendon,
7114 Oxford, 1986)] and Kuzuu [J. Phys. Soc. Jpn. 52, 3486 (1983)]. Here
7115 this theory is put to the test by comparing it against computer
7116 simulations. A Brownian dynamics simulation program was developed
7117 to follow the dynamics of the rods, with a length over a diameter
7118 ratio of 60, on the Smoluchowski time scale. The model accounts
7119 for excluded volume interactions between rods, but neglects hydrodynamic
7120 interactions. The self-rotational diffusion coefficients D-r(phi)
7121 of the rods were calculated by standard methods and by a new, more
7122 efficient method based on calculating average restoring torques.
7123 Collective decay of orientational order was calculated by means
7124 of equilibrium and nonequilibrium simulations. Our results show
7125 that, for the currently accessible volume fractions, the decay times
7126 in both cases are virtually identical. Moreover, the observed decay
7127 of diffusion coefficients with volume fraction is much quicker than
7128 predicted by the theory, which is attributed to an oversimplification
7129 of dynamic correlations in the theory. (c) 2005 American Institute
7130 of Physics.},
7131 Annote = {943DN Times Cited:3 Cited References Count:26},
7132 Author = {Y. G. Tao and W. K. {den Otter} and J. T. Padding and J. K. G. Dhont and W. J. Briels},
7133 Issn = {0021-9606},
7134 Journal = jcp,
7135 Month = {Jun 22},
7136 Number = 24,
7137 Pages = {-},
7138 Title = {Brownian dynamics simulations of the self- and collective rotational diffusion coefficients of rigid long thin rods},
7139 Uri = {<Go to ISI>://000230332400077},
7140 Volume = 122,
7141 Year = 2005}
7142
7143 @book{Tolman1979,
7144 Address = {New York},
7145 Author = {R.~C. Tolman},
7146 Chapter = 2,
7147 Pages = {19-22},
7148 Publisher = {Dover Publications, Inc.},
7149 Title = {The Principles of Statistical Mechanics},
7150 Year = 1979}
7151
7152 @article{Tu1995,
7153 Abstract = {We report a constant pressure and temperature molecular dynamics simulation
7154 of a fully hydrated liquid crystal (L(alpha) phase bilayer of dipalmitoylphosphatidylcholine
7155 at 50 degrees C and 28 water molecules/lipid. We have shown that
7156 the bilayer is stable throughout the 1550-ps simulation and have
7157 demonstrated convergence of the system dimensions. Several important
7158 aspects of the bilayer structure have been investigated and compared
7159 favorably with experimental results. For example, the average positions
7160 of specific carbon atoms along the bilayer normal agree well with
7161 neutron diffraction data, and the electron density profile is in
7162 accord with x-ray diffraction results. The hydrocarbon chain deuterium
7163 order parameters agree reasonably well with NMR results for the
7164 middles of the chains, but the simulation predicts too much order
7165 at the chain ends. In spite of the deviations in the order parameters,
7166 the hydrocarbon chain packing density appears to be essentially
7167 correct, inasmuch as the area/lipid and bilayer thickness are in
7168 agreement with the most refined experimental estimates. The deuterium
7169 order parameters for the glycerol and choline groups, as well as
7170 the phosphorus chemical shift anisotropy, are in qualitative agreement
7171 with those extracted from NMR measurements.},
7172 Annote = {Tv018 Times Cited:108 Cited References Count:34},
7173 Author = {K. Tu and D. J. Tobias and M. L. Klein},
7174 Issn = {0006-3495},
7175 Journal = bj,
7176 Month = {Dec},
7177 Number = 6,
7178 Pages = {2558-2562},
7179 Title = {Constant pressure and temperature molecular dynamics simulation of a fully hydrated liquid crystal phase dipalmitoylphosphatidylcholine bilayer},
7180 Uri = {<Go to ISI>://A1995TV01800037},
7181 Volume = 69,
7182 Year = 1995}
7183
7184 @article{Tuckerman1992,
7185 Abstract = {The Trotter factorization of the Liouville propagator is used to generate
7186 new reversible molecular dynamics integrators. This strategy is
7187 applied to derive reversible reference system propagator algorithms
7188 (RESPA) that greatly accelerate simulations of systems with a separation
7189 of time scales or with long range forces. The new algorithms have
7190 all of the advantages of previous RESPA integrators but are reversible,
7191 and more stable than those methods. These methods are applied to
7192 a set of paradigmatic systems and are shown to be superior to earlier
7193 methods. It is shown how the new RESPA methods are related to predictor-corrector
7194 integrators. Finally, we show how these methods can be used to accelerate
7195 the integration of the equations of motion of systems with Nose
7196 thermostats.},
7197 Annote = {Je891 Times Cited:680 Cited References Count:19},
7198 Author = {M. Tuckerman and B. J. Berne and G. J. Martyna},
7199 Issn = {0021-9606},
7200 Journal = jcp,
7201 Month = {Aug 1},
7202 Number = 3,
7203 Pages = {1990-2001},
7204 Title = {Reversible Multiple Time Scale Molecular-Dynamics},
7205 Uri = {<Go to ISI>://A1992JE89100044},
7206 Volume = 97,
7207 Year = 1992}
7208
7209 @book{Varadarajan1974,
7210 Address = {New York},
7211 Author = {V.S. Varadarajan},
7212 Publisher = {Prentice-Hall},
7213 Title = {Lie groups, Lie algebras, and their representations},
7214 Year = 1974}
7215
7216 @article{Vincent1995,
7217 Abstract = {We have implemented a portable parallel version of the macromolecular
7218 modeling package AMBER4. The message passing paradigm was used.
7219 All message passing constructs are compliant with the Message Passing
7220 Interface (MPI) standard. The molecular dynamics/minimization module
7221 MINMD and the free-energy perturbation module Gibbs have been implemented
7222 in parallel on a number of machines, including a Gray T3D, an IBM
7223 SP1/SP2, and a collection of networked workstations. In addition,
7224 the code has been tested with an MPI implementation from Argonne
7225 National Laboratories/Mississippi State University which runs on
7226 many parallel machines. The goal of this work is to decrease the
7227 amount of time required to perform molecular dynamics simulations.
7228 Performance results for a Lipid bilayer molecular dynamics simulation
7229 on a Gray T3D, an IBM SP1/SPZ and a Gray C90 are compared. (C) 1995
7230 by John Wiley & Sons, Inc.},
7231 Annote = {Ta403 Times Cited:16 Cited References Count:23},
7232 Author = {J. J. Vincent and K. M. Merz},
7233 Issn = {0192-8651},
7234 Journal = jcc,
7235 Month = {Nov},
7236 Number = 11,
7237 Pages = {1420-1427},
7238 Title = {A Highly Portable Parallel Implementation of Amber4 Using the Message-Passing Interface Standard},
7239 Uri = {<Go to ISI>://A1995TA40300009},
7240 Volume = 16,
7241 Year = 1995}
7242
7243 @article{Wegener1979,
7244 Author = {W.~A. Wegener, V.~J. Koester and R.~M. Dowben},
7245 Journal = {Proc. Natl. Acad. Sci.},
7246 Number = 12,
7247 Pages = {6356-6360},
7248 Title = {A general ellipsoid can not always serve as a modle for the rotational diffusion properties of arbitrary shaped rigid molecules},
7249 Volume = 76,
7250 Year = 1979}
7251
7252 @article{Wilson2006,
7253 Author = {G.~V. Wilson},
7254 Journal = {American Scientist},
7255 Title = {Where's the Real Bottleneck in Scientific Computing?},
7256 Volume = 94,
7257 Year = 2006}
7258
7259 @article{Withers2003,
7260 Abstract = {The effects of longitudinal quadrupole moments on the formation of
7261 liquid crystalline phases are studied by means of constant NPT Monte
7262 Carlo simulation methods. The popular Gay-Berne model mesogen is
7263 used as the reference fluid, which displays the phase sequences
7264 isotropic-smectic A-smectic B and isotropic-smectic B at high (T*=2.0)
7265 and low (T*=1.5) temperatures, respectively. With increasing quadrupole
7266 magnitude the smectic phases are observed to be stabilized with
7267 respect to the isotropic liquid, while the smectic B is destabilized
7268 with respect to the smectic A. At the lower temperature, a sufficiently
7269 large quadrupole magnitude results in the injection of the smectic
7270 A phase into the phase sequence and the replacement of the smectic
7271 B phase by the tilted smectic J phase. The nematic phase is also
7272 injected into the phase sequence at both temperatures considered,
7273 and ultimately for sufficiently large quadrupole magnitudes no coherent
7274 layered structures were observed. The stabilization of the smectic
7275 A phase supports the commonly held belief that, while the inclusion
7276 of polar groups is not a prerequisite for the formation of the smectic
7277 A phase, quadrupolar interactions help to increase the temperature
7278 and pressure range for which the smectic A phase is observed. The
7279 quality of the layered structure is worsened with increasing quadrupole
7280 magnitude. This behavior, along with the injection of the nematic
7281 phase into the phase sequence, indicate that the general tendency
7282 of the quadrupolar interactions is to destabilize the layered structure.
7283 A pressure dependence upon the smectic layer spacing is observed.
7284 This behavior is in much closer agreement with experimental findings
7285 than has been observed previously for nonpolar Gay-Berne and hard
7286 spherocylinder models. (C) 2003 American Institute of Physics.},
7287 Annote = {738EF Times Cited:3 Cited References Count:43},
7288 Author = {I. M. Withers},
7289 Issn = {0021-9606},
7290 Journal = jcp,
7291 Month = {Nov 15},
7292 Number = 19,
7293 Pages = {10209-10223},
7294 Title = {Effects of longitudinal quadrupoles on the phase behavior of a Gay-Berne fluid},
7295 Uri = {<Go to ISI>://000186273200027},
7296 Volume = 119,
7297 Year = 2003}
7298
7299 @article{Wolf1999,
7300 Abstract = {Based on a recent result showing that the net Coulomb potential in
7301 condensed ionic systems is rather short ranged, an exact and physically
7302 transparent method permitting the evaluation of the Coulomb potential
7303 by direct summation over the r(-1) Coulomb pair potential is presented.
7304 The key observation is that the problems encountered in determining
7305 the Coulomb energy by pairwise, spherically truncated r(-1) summation
7306 are a direct consequence of the fact that the system summed over
7307 is practically never neutral. A simple method is developed that
7308 achieves charge neutralization wherever the r(-1) pair potential
7309 is truncated. This enables the extraction of the Coulomb energy,
7310 forces, and stresses from a spherically truncated, usually charged
7311 environment in a manner that is independent of the grouping of the
7312 pair terms. The close connection of our approach with the Ewald
7313 method is demonstrated and exploited, providing an efficient method
7314 for the simulation of even highly disordered ionic systems by direct,
7315 pairwise r(-1) summation with spherical truncation at rather short
7316 range, i.e., a method which fully exploits the short-ranged nature
7317 of the interactions in ionic systems. The method is validated by
7318 simulations of crystals, liquids, and interfacial systems, such
7319 as free surfaces and grain boundaries. (C) 1999 American Institute
7320 of Physics. [S0021-9606(99)51517-1].},
7321 Annote = {189PD Times Cited:70 Cited References Count:34},
7322 Author = {D. Wolf and P. Keblinski and S. R. Phillpot and J. Eggebrecht},
7323 Issn = {0021-9606},
7324 Journal = jcp,
7325 Month = {May 1},
7326 Number = 17,
7327 Pages = {8254-8282},
7328 Title = {Exact method for the simulation of Coulombic systems by spherically truncated, pairwise r(-1) summation},
7329 Uri = {<Go to ISI>://000079913000008},
7330 Volume = 110,
7331 Year = 1999}
7332
7333 @article{Yoshida1990,
7334 Annote = {Ej798 Times Cited:492 Cited References Count:9},
7335 Author = {H. Yoshida},
7336 Issn = {0375-9601},
7337 Journal = {Physics Letters A},
7338 Month = {Nov 12},
7339 Number = {5-7},
7340 Pages = {262-268},
7341 Title = {Construction of Higher-Order Symplectic Integrators},
7342 Uri = {<Go to ISI>://A1990EJ79800009},
7343 Volume = 150,
7344 Year = 1990}
7345
7346 @article{Blum1972,
7347 Author = {L. Blum and A.~J. Torruella},
7348 Journal = jcp,
7349 Number = 1,
7350 Pages = {303-309},
7351 Title = {Computer simulations of bilayer membranes: Self-assembly and interfacial tension},
7352 Volume = 56,
7353 Year = 1972}
7354
7355 @article{Stone1978,
7356 Author = {A.~J. Stone},
7357 Journal = mp,
7358 Number = 1,
7359 Pages = {241-256},
7360 Title = {The description of bimolecular potentials, forces and torques: the S and V function expansions},
7361 Volume = 36,
7362 Year = 1978}
7363
7364 @article{Berardi2003,
7365 Author = {R. Berardi, M. Cecchini and C. Zannoni},
7366 Journal = jcp,
7367 Number = 18,
7368 Pages = {9933-9946},
7369 Title = {A Monte Carlo study of the chiral columnar organizations of dissymmetric discotic mesogens},
7370 Volume = 119,
7371 Year = 2003}
7372
7373 @article{Beard2000,
7374 Author = {D. A. Beard and T. Schlick},
7375 Journal = jcp,
7376 Number = 17,
7377 Pages = {7313-7322},
7378 Title = {Inertial Stochastic Dynamics. I. Long-time-step Methods for Langevin Dynamics},
7379 Volume = 112,
7380 Year = 2000}
7381
7382 @book{Hirsch1997,
7383 Address = {New York},
7384 Author = {M.W. Hirsch},
7385 Publisher = {Springer},
7386 Title = {Differential Topology},
7387 Year = 1997}
7388
7389 @book{Jost2002,
7390 Address = {Berlin},
7391 Author = {J. Jost},
7392 Publisher = {Springer-Verlag},
7393 Title = {Riemannian Geometry and Geometric Analysis},
7394 Year = 2002}
7395
7396 @book{McDuff1998,
7397 Address = {Oxford},
7398 Author = {D. McDuff and D. Salamon},
7399 Publisher = {Oxford Mathematical Monographs},
7400 Title = {Introduction to Symplectic Topology},
7401 Year = 1998}
7402
7403 @article{Matubayasi1999,
7404 Author = {N. Matubayasi and M. Nakahara},
7405 Journal = jcp,
7406 Number = 7,
7407 Pages = {3291-3301},
7408 Title = {Reversible molecular dynamics for rigid bodies and hybrid Monte Carlo},
7409 Volume = 110,
7410 Year = 1999}
7411
7412 @article{Miller2002,
7413 Author = {T.F. Miller III, M. Eleftheriou},
7414 Journal = jcp,
7415 Number = 20,
7416 Pages = {8649-8659},
7417 Title = {Symplectic quaternion scheme for biophysical molecular dynamics},
7418 Volume = 116,
7419 Year = 1999}
7420
7421 @article{McMillan1971,
7422 Author = {W.L. McMillan},
7423 Journal = jcp,
7424 Number = 3,
7425 Pages = {1238-1246},
7426 Title = {Simple Molecular Model for the Smectic A Phase of Liquid Crystals},
7427 Volume = 4,
7428 Year = 1971}
7429
7430 @article{Gilmore1974,
7431 Author = {R. Gilmore},
7432 Journal = {Journal of Mathematical Physics},
7433 Number = 12,
7434 Pages = {2090-2092},
7435 Title = {Baker-Campbell-Hausdorff Formulas},
7436 Volume = 15,
7437 Year = 1974}
7438
7439 @article{Strang1968,
7440 Author = {G. Strang},
7441 Journal = {SIAM Journal on Numerical Analysis},
7442 Number = 3,
7443 Pages = {506-517},
7444 Title = {On the construction and comparision of difference schemes},
7445 Volume = 5,
7446 Year = 1968}
7447
7448 @article{Trotter1959,
7449 Author = {H.F. Trotter},
7450 Journal = {SIAM Journal on Numerical Analysis},
7451 Number = 14,
7452 Pages = {545-551},
7453 Title = {On the product of semi-groups of operators},
7454 Volume = 10,
7455 Year = 1959}
7456
7457 @article{Cartwright1992,
7458 Author = {J.H.E. Cartwright and O. Piro},
7459 Journal = {International Journal of Bifurcation and Chaos},
7460 Number = 3,
7461 Pages = {427-449},
7462 Title = {The Dynamics of Runge-Kutta Methods},
7463 Volume = 2,
7464 Year = 1992}
7465
7466 @article{HuseyinKaya07012005,
7467 Abstract = {It has been demonstrated that a "near-Levinthal" cooperative mechanism, whereby the common G[o] interaction scheme is augmented by an extra favorability for the native state as a whole, can lead to apparent two-state folding/unfolding kinetics over a broad range of native stabilities in lattice models of proteins. Here such a mechanism is shown to be generalizable to a simplified continuum (off-lattice) Langevin dynamics model with a C{alpha} protein chain representation, with the resulting chevron plots exhibiting an extended quasilinear regime reminiscent of that of apparent two-state real proteins. Similarly high degrees of cooperativity are possible in G[o]-like continuum models with rudimentary pairwise desolvation barriers as well. In these models, cooperativity increases with increasing desolvation barrier height, suggesting strongly that two-state-like folding/unfolding kinetics would be achievable when the pairwise desolvation barrier becomes sufficiently high. Besides cooperativity, another generic folding property of interest that has emerged from published experiments on several apparent two-state proteins is that their folding relaxation under constant native stability (isostability) conditions is essentially Arrhenius, entailing high intrinsic enthalpic folding barriers of [~]17-30 kcal/mol. Based on a new analysis of published data on barnase, here we propose that a similar property should also apply to a certain class of non-two-state proteins that fold with chevron rollovers. However, several continuum G[o]-like constructs considered here fail to predict any significant intrinsic enthalpic folding barrier under isostability conditions; thus the physical origin of such barriers in real proteins remains to be elucidated.
7468 },
7469 Author = {Kaya, Huseyin and Liu, Zhirong and Chan, Hue Sun},
7470 Doi = {10.1529/biophysj.104.057471},
7471 Eprint = {http://www.biophysj.org/cgi/reprint/89/1/520.pdf},
7472 Journal = {Biophys. J.},
7473 Number = 1,
7474 Pages = {520-535},
7475 Title = {{Chevron Behavior and Isostable Enthalpic Barriers in Protein Folding: Successes and Limitations of Simple Go-like Modeling}},
7476 Url = {http://www.biophysj.org/cgi/content/abstract/89/1/520},
7477 Volume = 89,
7478 Year = 2005,
7479 Bdsk-Url-1 = {http://www.biophysj.org/cgi/content/abstract/89/1/520},
7480 Bdsk-Url-2 = {http://dx.doi.org/10.1529/biophysj.104.057471}}
7481
7482 @article{JoseGarciadelaTorre02012000,
7483 Abstract = {The solution properties, including hydrodynamic quantities and the radius of gyration, of globular proteins are calculated from their detailed, atomic-level structure, using bead-modeling methodologies described in our previous article (Carrasco and Garcia de la Torre, 1999, Biophys. J. 76:3044-3057). We review how this goal has been pursued by other authors in the past. Our procedure starts from a list of atomic coordinates, from which we build a primary hydrodynamic model by replacing nonhydrogen atoms with spherical elements of some fixed radius. The resulting particle, consisting of overlapping spheres, is in turn represented by a shell model treated as described in our previous work. We have applied this procedure to a set of 13 proteins. For each protein, the atomic element radius is adjusted, to fit all of the hydrodynamic properties, taking values close to 3 A, with deviations that fall within the error of experimental data. Some differences are found in the atomic element radius found for each protein, which can be explained in terms of protein hydration. A computational shortcut makes the procedure feasible, even in personal computers. All of the model-building and calculations are carried out with a HYDROPRO public-domain computer program.
7484 },
7485 Author = {{Garc\'{i}a de la Torre}, Jose and Huertas, Maria L. and Carrasco, Beatriz},
7486 Eprint = {http://www.biophysj.org/cgi/reprint/78/2/719.pdf},
7487 Journal = bj,
7488 Number = {2},
7489 Pages = {719-730},
7490 Title = {{Calculation of Hydrodynamic Properties of Globular Proteins from Their Atomic-Level Structure}},
7491 Url = {http://www.biophysj.org/cgi/content/abstract/78/2/719},
7492 Volume = {78},
7493 Year = {2000},
7494 Bdsk-Url-1 = {http://www.biophysj.org/cgi/content/abstract/78/2/719}}
7495
7496 @article{GarciadelaTorreJ2002,
7497 Affiliation = {Departamento de Qu{\'\i}mica F{\'\i}sica, Facultad de Qu{\'\i}mica, Universidad de Murcia, 30071 Murcia, Spain},
7498 Author = {{Garc\'{i}a de la Torre}, Jose and Carrasco, B.},
7499 Journal = {Biopolymers},
7500 Number = {3},
7501 Pages = {163-167},
7502 Title = {Hydrodynamic Properties of Rigid Macromolecules Composed of Ellipsoidal and Cylindrical Subunits},
7503 Volume = {63},
7504 Year = {2002}}