「Formula for field dependent mobility」：修訂間差異
跳至導覽
跳至搜尋
已建立頁面，內容為 " For semiconductor material, there are many field dependent mobility model. It is hard to get one equations fitted with all materials. Hence, the field dependent mo..." |
無編輯摘要 |
||
| 第5行： | 第5行： | ||
type: 1 | type: 1 | ||
<math> | <math> v = \frac{\vec{E} p_{1} + p_{2} \left( \frac{\vec{E}}{p_{3}} \right)^{p_4} }{ 1+ \left( \frac{\vec{E}}{p_{3}} \right)^{p_{4}} + p_{5}\left( \frac{\vec{E}}{p_{3}} \right)^{p_{6}} } </math> | ||
於 2021年7月20日 (二) 01:18 的修訂
For semiconductor material, there are many field dependent mobility model. It is hard to get one equations fitted with all materials. Hence, the field dependent mobility model is case dependent. Usually it can be described by model fitting. However, we still define some equations that people proposed to be used in DDCC. For 2D-DDCC, the field dependent mobility model can be defined by different type
type: 1