======Equation of motion====== 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} =====Fermionic Field Operator===== The EoM for the electronic creation and annihilation operator is \begin{equation} \frac{\partial}{\partial t} \hat{\Psi}_\text{H} (x,t) = \dots \end{equation} according to the calculation [[forcebalance:calculation:EoM fermionic field operator|here]]. Condition: \begin{equation} \nu (\vec{r},\vec{r}^\prime) = \nu (\vec{r}^\prime,\vec{r}) \end{equation} =====Particle Number Operator===== The EoM of the particle number operator \begin{equation} \frac{\partial}{\partial t} \hat{n}_\text{H}= \dots \end{equation} is of the form of a [[forcebalance:continuity equation]]. The calculation is done [[forcebalance:calculation:EoM particle number operator|here]]. =====Current Density Operator===== Wtih the help of the EoM of the fermionic field operator, the EoM for the current density operator $J(x,t)$ becomes \begin{equation} \frac{\partial}{\partial t} \hat{J}_\text{H} (x,t) = \frac{\partial}{\partial t} \hat{j}_\text{H} (x,t) + \frac{\partial}{\partial t} \hat{j}_\text{d,H} (x,t) = \dots + \dots \quad . \end{equation} FIXME Insert Link to para and diramagnetic definitions This holds for symmetric correlation potentials \begin{equation} \nu (\vec{r},\vec{r}^\prime) = \nu (\vec{r}^\prime,\vec{r}) \end{equation} and (Do a page where I discuss where this occurs) \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 current density operator|here]].