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{|border="0" align="center"
|<math> \begin{array}{rcl} \mathbf{P} & \equiv & \sum_i m_i\mathbf{v}_ i = \mathrm{Const.} \\ \mathbf{L} & \equiv & \sum_i \mathbf{r}_i \times m_i\mathbf{v}_i = \mathrm{Const.} \end{array}, </math>
|<math> \begin{array}{rcl} \mathbf{P} & \equiv & \sum_i m_i\mathbf{v}_ i = \mathrm{Const.} \\ \mathbf{L} & \equiv & \sum_i \mathbf{r}_i \times m_i\mathbf{v}_i = \mathrm{Const.} \end{array}, </math>
|}

{| class="wikitable" style="margin: 1em auto 1em auto"
|+ '''Table 1.''' Elastic constants of DC Si. Potential Model : SW
|-
! T (K) !! C<sub>11</sub> !! C<sub>22</sub> !! C<sub>33</sub> !! C<sub>12</sub> !! C<sub>13</sub> !! C<sub>23</sub> !! C<sub>44</sub> !! C<sub>55</sub> || C<sub>66</sub>
|-
! 300
| 149.41 || 149.36 || 149.45 || 76.26 || 76.18 || 76.24 || 62.45 || 75.00 || 54.93
|-
! 625
| 146.35 || 146.29 || 146.35 || 75.80 || 75.77 || 75.71 || 53.72 || 50.03 || 46.98
|-
! 888
| 142.74 || 142.86 || 142.84 || 75.07 || 75.17 || 74.99 || 60.78 || 53.54 || 56.76
|-
! 1164
| 139.11 || 139.06 || 139.29 || 74.28 || 74.33 || 74.27 || 47.30 || 60.86 || 51.17
|-
! 1477
| 135.02 || 134.84 || 134.69 || 73.84 || 73.85 || 73.80 || 44.96 || 41.41 || 47.66
|}
|}

Revision as of 21:49, 14 July 2009

Manual 08 for MD++
Computing elastic constants at nonzero temperature

Keonwook Kang, Seunghwa Ryu and Wei Cai

Jul 08 , 2009



In the previous manual, the elastic constants of bulk silicon of diamond cubic structure are computed at 0 K. In this manual, we compute the elastic constants at nonzero finite temperature using fluctuation-dissipation theorem.

Table 1. Elastic constants of DC Si. Potential Model : SW
T (K) C11 C22 C33 C12 C13 C23 C44 C55 C66
300 149.41 149.36 149.45 76.26 76.18 76.24 62.45 75.00 54.93
625 146.35 146.29 146.35 75.80 75.77 75.71 53.72 50.03 46.98
888 142.74 142.86 142.84 75.07 75.17 74.99 60.78 53.54 56.76
1164 139.11 139.06 139.29 74.28 74.33 74.27 47.30 60.86 51.17
1477 135.02 134.84 134.69 73.84 73.85 73.80 44.96 41.41 47.66