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\usepackage{setspace} |
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\usepackage{tabularx} |
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\usepackage{longtable} |
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\lstset{language=C++,frame=TB,basicstyle=\footnotesize, % |
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captionpos=b, % |
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xleftmargin=0.1in,xrightmargin=0.1in, |
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keywordstyle=\footnotesize, breaklines=true, |
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abovecaptionskip=0.5cm, belowcaptionskip=0.5cm |
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} |
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> |
\lstset{language=C,frame=TB,basicstyle=\small\ttfamily, % |
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> |
xleftmargin=0in, xrightmargin=0in, captionpos=b,% breaklines=true, % |
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abovecaptionskip=0.5cm, belowcaptionskip=0.5cm} |
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\renewcommand{\lstlistingname}{Scheme} |
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\includeonly{preview} |
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|
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\begin{document} |
| 68 |
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colleagues, I developed a new molecular dynamics framework capable |
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of performing simulation on systems with orientational degrees of |
| 70 |
|
freedom in a variety of ensembles. Using this new package, I studied |
| 71 |
< |
the structure, the dynamics and transport properties of the |
| 72 |
< |
biological membranes as well as the the phase behavior of banana |
| 73 |
< |
shaped liquid crystals. A new Langevin dynamics algorithm for |
| 74 |
< |
arbitrary rigid particles is proposed to mimic solvent effects which |
| 75 |
< |
may eventually expand the time scale of the simulation. |
| 71 |
> |
the structure, dynamics and transport properties of the biological |
| 72 |
> |
membranes as well as the the phase behavior of banana shaped liquid |
| 73 |
> |
crystals. A new Langevin dynamics algorithm for arbitrary rigid |
| 74 |
> |
particles is also presented to mimic solvent effects which may |
| 75 |
> |
eventually expand the time scale of the simulation. |
| 76 |
|
|
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\end{abstract} |
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|
