debugging

source/Charge.tex

 \begin{modsig}{Charge}
   \gimport[smglom/arithmetics]{realarith}
-  \gimport{DeviceGeometry}
   \gimport{DopingProfile}
   \gimport{PoissonParameters}
   \gimport{DensityElectrons}

source/ContinuityEquationElectrons.tex

 \begin{modsig}{ContinuityEquationElectrons}
   \gimport{CurrentElectrons}
-  \gimport{DensityHoles}
   \gimport{FermiPotentialHoles}
   \gimport{Recombination}
-  \gimport{ElectrostaticPotential}
 \end{modsig}
 
 %%% Local Variables:

source/ContinuityEquationHoles.tex

 \begin{modsig}{ContinuityEquationHoles}
   \gimport{CurrentHoles}
-  \gimport{DensityElectrons}
   \gimport{FermiPotentialElectrons}
   \gimport{Recombination}
-  \gimport{ElectrostaticPotential}
 \end{modsig}
 
 %%% Local Variables:

source/Device.tex

 \begin{modsig}{Device}
+    \symi{device}
+    \symii{device}{property}
 \end{modsig}
 %%% Local Variables:
 %%% mode: latex

source/DopingProfile.tex

 \begin{modsig}{DopingProfile}
   \gimport{DeviceGeometry}
-  \gimport[smglom/sets]{functions}
-  \gimport[smglom/arithmetics]{realnumbers}
  
   \symdef[name=doping-profile]{DopingProfile}{C}
   \symtest{DopingProfile}{\DopingProfile}

source/FermiPotentialElectrons.en.tex

 \begin{mhmodnl}{FermiPotentialElectrons}{en}
 \begin{definition}
-  The \defiii{Fermi}{Potential}{Electrons} usually denoted by $\QFPnOp$ is a function
+  The \defiii{Fermi}{potential}{electrons} usually denoted by $\QFPnOp$ is a function
   describing the variation of the quasi-Fermi potentials of the electrons across the
   domain $\DeviceDomain$.  It is linked to the quasi-Fermi level of the electrons which
   controls the occupation of the conduction band and is a measure for the electron density

source/OneDimDeviceGeometry.tex

 \begin{modsig}{OneDimDeviceGeometry}
   \gimport{OneDimDevice}
-  \gimport{DeviceGeometry}
 \end{modsig}
 
 %%% Local Variables:

source/TwoDimDeviceGeometry.tex

 \begin{modsig}{TwoDimDeviceGeometry}
   \gimport{TwoDimDevice}
-  \gimport{DeviceGeometry}
   \gimport{PDERegularDomain}
 \end{modsig}