| 472 |
|
density in low speed is confidently smaller than ideal distribution; |
| 473 |
|
in low temperature slabs, probability density in high speed is smaller |
| 474 |
|
than ideal. This phenomenon is observable even in our relatively low |
| 475 |
< |
swpping rate simulations. And this deviation could also leads to |
| 475 |
> |
swapping rate simulations. And this deviation could also leads to |
| 476 |
|
deviation of distribution of velocity in various dimensions. One |
| 477 |
|
feature of these deviated distribution is that in high temperature |
| 478 |
|
slab, the ideal Gaussian peak was changed into a relatively flat |
| 482 |
|
\includegraphics[width=\linewidth]{histSwap} |
| 483 |
|
\caption{Speed distribution for thermal conductivity using swapping RNEMD.} |
| 484 |
|
\label{histSwap} |
| 485 |
+ |
\end{figure} |
| 486 |
+ |
|
| 487 |
+ |
\begin{figure} |
| 488 |
+ |
\includegraphics[width=\linewidth]{histScale} |
| 489 |
+ |
\caption{Speed distribution for thermal conductivity using scaling RNEMD.} |
| 490 |
+ |
\label{histScale} |
| 491 |
|
\end{figure} |
| 492 |
|
|
| 493 |
|
\subsection{Interfaciel Thermal Conductivity} |
