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forcebalance:equation_of_moiton [2023/11/21 13:45] – created cjoensforcebalance:equation_of_moiton [2023/11/21 14:03] (current) cjoens
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-======Equation of motion====== +======DeleteMe======
-The equations of motion are derived here with the help of the [[QM representations|Heisenberg EoM]]. +
-Starting in the [[QM representations|Heisenberg picture]] the time evolution of an operator is +
-\begin{equation} +
-  \frac{\partial}{\partial t} \hat{O}_\text{H} (x,t) +
-  = +
-  \left[ +
-    \hat{O}_\text{H} (x,t) +
-  , +
-    \hat{H}_\text{H} (t) +
-  \right] +
-  + +
-  \left( +
-    \frac{\partial}{\partial t} \hat{O}_\text{S} (x) +
-  \right)_\text{H} +
-  \quad . +
-\end{equation} +
-Under the following conditions, the EoM for the electron current $J(x,t)$ becomes +
-\begin{equation} +
-  \frac{\partial}{\partial t} J (x,t) +
-  = +
-  \dots +
-  \quat . +
-\end{equation} +
-This holds for +
-\begin{equation} +
-  \nu (\vec{r},\vec{r}^\prime) +
-  = +
-  \nu (\vec{r},\vec{r}^\prime) +
-\end{equation} +
-and +
-\begin{equation} +
-  \frac{\partial}{\partial t} +
-  \frac{\partial}{\partial k} +
-  = +
-  \frac{\partial}{\partial k} +
-  \frac{\partial}{\partial t} +
-  \quad . +
-\end{equation} +
-The calculation can be found [[forcebalance:calculation:EoM electron current|here]].+
forcebalance/equation_of_moiton.1700570752.txt.gz · Last modified: 2023/11/21 13:45 by cjoens

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