579 |
|
solvent and capping agent (or without capping agent) at |
580 |
|
$\langle T\rangle\sim$200K. (D stands for deuterated solvent |
581 |
|
or capping agent molecules; ``Avg.'' denotes results that are |
582 |
< |
averages of simulations under different applied thermal flux values $(J_z)$. Error |
583 |
< |
estimates are indicated in parentheses.)} |
582 |
> |
averages of simulations under different applied thermal flux |
583 |
> |
values $(J_z)$. Error estimates are indicated in |
584 |
> |
parentheses.)} |
585 |
|
|
586 |
|
\begin{tabular}{llccc} |
587 |
|
\hline\hline |
866 |
|
shown as in Figure \ref{specAu}. Regardless of the presence of |
867 |
|
solvent, the gold surfaces which are covered by butanethiol molecules |
868 |
|
exhibit an additional peak observed at a frequency of |
869 |
< |
$\sim$170cm$^{-1}$. We attribute this peak to the S-Au bonding |
869 |
> |
$\sim$165cm$^{-1}$. We attribute this peak to the S-Au bonding |
870 |
|
vibration. This vibration enables efficient thermal coupling of the |
871 |
|
surface Au layer to the capping agents. Therefore, in our simulations, |
872 |
|
the Au / S interfaces do not appear to be the primary barrier to |
877 |
|
\includegraphics[width=\linewidth]{vibration} |
878 |
|
\caption{Vibrational power spectra for gold in different solvent |
879 |
|
environments. The presence of the butanethiol capping molecules |
880 |
< |
adds a vibrational peak at $\sim$170cm$^{-1}$.} |
880 |
> |
adds a vibrational peak at $\sim$165cm$^{-1}$. The butanethiol |
881 |
> |
spectra exhibit a corresponding peak.} |
882 |
|
\label{specAu} |
883 |
|
\end{figure} |
884 |
|
|
885 |
|
Also in this figure, we show the vibrational power spectrum for the |
886 |
|
bound butanethiol molecules, which also exhibits the same |
887 |
< |
$\sim$170cm$^{-1}$ peak. |
887 |
> |
$\sim$165cm$^{-1}$ peak. |
888 |
|
|
889 |
|
\subsection{Overlap of power spectra} |
890 |
|
A comparison of the results obtained from the two different organic |