forcebalance:equation_of_moiton
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| forcebalance:equation_of_moiton [2023/11/21 13:45] – created cjoens | forcebalance: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}, | + | |
| - | = | + | |
| - | \nu (\vec{r}, | + | |
| - | \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: | + | |
forcebalance/equation_of_moiton.1700570752.txt.gz · Last modified: 2023/11/21 13:45 by cjoens