590 |
|
significantly smaller than experimental value by an order of more than |
591 |
|
100. It has been verified that this difference is mainly attributed to |
592 |
|
the lack of electron interaction representation in these force field |
593 |
< |
parameters. Richardson {\it et al.}\cite{ISI:A1992HX37800010} used EAM |
593 |
> |
parameters. Richardson {\it et al.}\cite{Clancy:1992} used EAM |
594 |
|
force field parameters in their metal thermal conductivity |
595 |
|
calculations. The Non-Equilibrium MD method they employed in their |
596 |
|
simulations produced comparable results to ours. As Zhang {\it et |