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1 chrisfen 2987 \chapter{\label{chap:conclusion}CONCLUSION}
2    
3 chrisfen 3001 The preceding chapters and included appendices discuss the primary
4     aspects of the research I have performed and been involved with over
5     the last several years. Rather than presenting the topics in a
6     chronological fashion, they were arranged to form a series where the
7     later topics apply and extend the findings of the former topics. This
8     layout is more instructive and provides a more cohesive progression of
9     research efforts.
10    
11     The first chapter laid out the foundation from which the research in
12     the later chapters is built upon, primarily the technique of molecular
13     dynamics. This chapter also introduces {\sc oopse}, the object
14     oriented parallel simulation engine, the unified code-base developed in
15     our lab for performing molecular simulations. Starting out as a
16     collection of separate programs written by different group members,
17     {\sc oopse} has developed into one of the few parallel molecular
18     dynamics packages capable of accurately integrating rigid bodies,
19     point multipoles, and metallic potentials.\cite{Meineke05}
20    
21     The second chapter discussed correction techniques for handling the
22     long-ranged electrostatic interactions common in molecular
23     simulations, in particular our shifted-force ({\sc sf}) modification
24     of the damped shifted Coulombic summation method developed by Wolf
25     {\it et al.}\cite{Wolf99} In the work outlined here, we showed {\sc
26 chrisfen 3023 sf} to be nearly equivalent to the more prevalent Ewald summation in
27 chrisfen 3001 simulations of condensed phases, and since it is pairwise, it scales
28     as $\mathcal{O}(N)$ and lacks periodicity artifacts introduced through
29     heavy reliance on the reciprocal-space portion of the Ewald sum. We
30     extended the electrostatic damping technique used with {\sc sf} beyond
31     simple charge-charge interactions to include point-multipoles, and we
32     also identified optimal damping parameter settings to ensure proper
33     depiction of the dielectric behavior of molecular systems. Presenting
34     this technique early enables us to apply it in the systems discussed
35     in the later chapters and show how it can improve the quality of
36     various molecular simulations.
37    
38     The third chapter focused on simple water models, specifically the
39     single-point soft sticky dipole (SSD) model for water. We implemented
40     this model and realized that we need to reparametrize it in order to
41     use it in our simulations. This lead to the development of SSD/RF and
42     SSD/E, new variants of the SSD model optimized for simulations with
43     and without a reaction field correction. These new single-point models
44     are more efficient than the common multi-point partial charge models
45     and better capture the dynamic properties of water. We also showed
46     that SSD/RF can be successfully used with damped {\sc sf} through our
47     multipolar extension of the technique. For the sake of completeness,
48     we also developed the two-point tetrahedrally restructured elongated
49     dipole (TRED) water model, which is optimized for use with the damped
50     {\sc sf} technique. Though there remain some algorithmic complexities
51     that need to be addressed (logic for neglecting charge-quadrupole
52     interactions between other TRED molecules) to use this model in
53     general simulations, it is approximately twice as efficient as the
54     commonly used three-point charge water models (i.e. TIP3P and
55     SPC/E). This work succeeds in extending the limits of the
56     computational efficiency of water models that can capture the
57     thermodynamic and dynamic properties of liquid water.
58    
59     The final chapter deals with a unique polymorph of ice that we
60     discovered while performing water simulations with the fast simple
61 chrisfen 3042 water models discussed in chapter~\ref{chap:water}. This form of ice,
62 chrisfen 3001 which we called ``imaginary ice'' (Ice-$i$), has a low-density
63     structure which is different from any known polymorph from either
64     experiment or other simulations. The free energy analysis performed
65     here shows that this structure is in fact the thermodynamically
66     preferred form of ice for both the single-point and commonly used
67     multi-point water models under the chosen simulation conditions. We
68     then showed that inclusion of electrostatic corrections is necessary
69     to obtain more realistic results; however, the free energies of the
70     various polymorphs (both imaginary and real) in many of these models
71     was shown to be so similar that choice of system properties, like the
72     volume in $NVT$ simulations, will directly influence the expressed ice
73     polymorph. This work shows that researchers ought to be wary of using
74     these simplistic water models in the study of complex phase behavior
75     where the choice of a water model that includes many-body effects,
76     such as polarizability, might be more appropriate.
77    
78     The work presented in this dissertation includes advancements in
79     simulation techniques, improved molecular models, and applications of
80     both in simulations of novel molecular systems. In addition to
81     answering interesting questions related to these topics, this work
82     opens up new routes which other researchers can utilize to extend and
83     improve their own work. Though specific in focus, through pathways
84     such as these, this work can gain wider utility and expand our
85     understanding of natural physical and chemical processes.