@@ -320,7 +320,7 @@ See Table~\ref{fieldsolvercmd} for a summary of the Fieldsolver command.

\begin{center}

\caption{Fieldsolver command summary}

\label{tab:fieldsolvercmd}

\begin{tabular}{|l|p{0.6\textwidth}|l|}

\begin{tabular}{|l|l|}

\hline

\tabhead Command & Purpose \\

\hline

...

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@@ -440,7 +440,7 @@ The behavior of the preconditioner can be: \texttt{STD}\index{PRECMODE!STD}, \te

Suppose $\mathrm{d} E$ the energy spread in the particle bunch is to large, the electrostatic approximation is no longer valid.

One solution to that problem is to introduce $k$ energy bins and perform $k$ separate field solves

in which $\mathrm{d} E$ is again small and hence the electrostatic approximation valid. In case of a cyclotron

see~Section~\ref{cyclotron} the number of energy bins must be at minimum the number of neighboring bunches (\texttt{NNEIGHBB}) i.e. $\text{\texttt{ENBINS}}\le\text{\texttt{NNEIGHBB}}$.

see~Section~\ref{cyclotron} the number of energy bins must be at minimum the number of neighboring bunches (\texttt{NNEIGHBB}) i.e. $\mathrm{ENBINS}\lemathrm{NNEIGHBB}$.

The variable \texttt{MINSTEPFORREBIN} defines the number of integration step that have to pass until all energy bins are merged into one.

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@@ -460,7 +460,7 @@ simulation one requires following ingredients:

\begin{table}[ht] \footnotesize

\begin{center}

\caption{Mesh-refinement strategies}

\caption{Meshrefinement strategies}

\label{tab:tagging_strategies}

\begin{tabular}{|l|p{0.6\textwidth}|}

\hline

...

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@@ -470,16 +470,16 @@ simulation one requires following ingredients:

scaling factor \texttt{AMR\_SCALING}\\

\texttt{EFIELD}& Mark each cell if the electric field component of any direction satisfies

$E^{level}_{d, cell}\ge\alpha\max E_{d}^{level}$, where $d=x, y, z$ and $\alpha\in[0, 1]$ is the scaling factor

\texttt{AMR\_SCALING}\\

\texttt{AMR\_SCALING}&\\

\texttt{MOMENTA}& It performs a loop over all particles of a level and computes the dot product of the momenta.\ Every

cell that contains a particle with $||\mathbf{p}|| \ge\alpha\max_{level} ||\mathbf{p}||$ is refined.\ The scalar $\alpha\in[0, 1]$

is a user-defined value \texttt{AMR\_SCALING}. \\

\texttt{CHARGE\_DENSITY}& If the charge density of a cell is greater or equal to the value specified with

\texttt{AMD\_DENSITY} the cell is tagged for refinement\\

\texttt{MIN\_NUM\_PARTICLES}& Cells with equal or more particles are refined.\ The bound is specified with

\texttt{AMR\_MIN\_NUM\_PART}\\

\texttt{AMR\_MIN\_NUM\_PART}&\\

\texttt{MAX\_NUM\_PARTICLES}& Cells with equal or less particles are refined.\ The bound is specified with