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that must be tuned to give experimentally relevant simulations. |
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\begin{figure}[htbp] |
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\centering |
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< |
\includegraphics[width=\linewidth]{images/stochbound.pdf} |
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> |
\includegraphics[width=5in]{images/stochbound.pdf} |
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\caption{Methodology used to mimic the experimental cooling conditions |
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of a hot nanoparticle surrounded by a solvent. Atoms in the core of |
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the particle evolved under Newtonian dynamics, while atoms that were |
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in the outer skin of the particle evolved under Langevin dynamics. |
71 |
< |
The radial cutoff between the two dynamical regions was set to 4 {\AA} |
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< |
smaller than the original radius of the liquid droplet.} |
71 |
> |
The radius of the spherical region operating under Newtonian dynamics, |
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> |
$r_\textrm{Newton}$ was set to be 4 {\AA} smaller than the original |
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> |
radius ($R$) of the liquid droplet.} |
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|
\label{fig:langevinSketch} |
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\end{figure} |
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|
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|
|
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|
\begin{figure}[htbp] |
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\centering |
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< |
\includegraphics[width=\linewidth]{images/cooling_plot.pdf} |
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> |
\includegraphics[width=5in]{images/cooling_plot.pdf} |
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\caption{Thermal cooling curves obtained from the inverse Laplace |
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transform heat model in Eq. \ref{eq:laplacetransform} (solid line) as |
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well as from molecular dynamics simulations (circles). Effective |
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|
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|
\begin{figure}[htbp] |
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\centering |
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< |
\includegraphics[width=\linewidth]{images/cross_section_array.jpg} |
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> |
\includegraphics[width=5in]{images/cross_section_array.jpg} |
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\caption{Cutaway views of 30 \AA\ Ag-Cu nanoparticle structures for |
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random alloy (top) and Cu (core) / Ag (shell) initial conditions |
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(bottom). Shown from left to right are the crystalline, liquid |
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droplet, and final glassy bead configurations.} |
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< |
\label{fig:q6} |
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> |
\label{fig:cross_sections} |
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\end{figure} |