debugging with pin

source/DensityElectrons.en.tex

 \begin{mhmodnl}{DensityElectrons}{en}
 \begin{definition}
-  Formula for the electron density for the Boltzmann approximation.
+  Formula for the \defii{electron}{density} for the Boltzmann approximation.
 \end{definition}
 \end{mhmodnl}
 

source/ElectrostaticPotential.en.tex

 \begin{mhmodnl}{ElectrostaticPotential}{en}
   \begin{definition}
-    Spatial variation of the electrostatic potential, usually denoted by
+    Spatial variation of the \defii{electrostatic}{potential}, usually denoted by
     $\ElectrostaticPotential$.
   \end{definition}
 \end{mhmodnl}

source/ElectrostaticPotential.tex

-I\begin{modsig}{ElectrostaticPotential}
+\begin{modsig}{ElectrostaticPotential}
   \gimport{DeviceGeometry}
 
   \symdef[name=electrostatic-potential]{ElectrostaticPotential}{\Psi}

source/FermiPotentialElectrons.en.tex

 \begin{mhmodnl}{FermiPotentialElectrons}{en}
 \begin{definition}
-  The \defiii{Fermi}{Potential}{Electrons} usually denoted by $\Fn$ is a function
+  The \defiii{Fermi}{Potential}{Electrons} usually denoted by $\QFPn$ 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/FermiPotentialElectrons.tex

@@ -2,9 +2,9 @@
 \begin{modsig}{FermiPotentialElectrons}
   \gimport{DeviceGeometry}
   
-  \symdef[name=quasi-Fermi-potential]{FnOp}{\varphi_n}
-  \symdef[name=quasi-Fermi-potential]{Fn}[1]{\prefix\FnOp{#1}}
-  \symtest{Fn}{\Fn{x}}
+  \symdef[name=quasi-Fermi-potential]{QFPnOp}{\varphi_n}
+  \symdef[name=quasi-Fermi-potential]{QFPn}[1]{\prefix{\QFPnOp}{#1}}
+  \symtest{QFPn}{\QFPn{x}}
 \end{modsig}
 
 %%% Local Variables:

source/FermiPotentialHoles.en.tex

 \begin{mhmodnl}{FermiPotentialHoles}{en}
 \begin{definition}
-  The \defiii{Fermi}{Potential}{Holes} usually denoted by $\Fp$ is a function describing
+  The \defiii{Fermi}{Potential}{Holes} usually denoted by $\QFPp$ is a function describing
   the variation of the quasi-Fermi potentials of the holes across the domain
   $\DeviceDomain$.  It is linked to the quasi-Fermi level of the holes which controls the
   occupation of the valance band. Its gradient is the driving force of the hole current.

source/FermiPotentialHoles.tex

 \begin{modsig}{FermiPotentialHoles}
   \gimport{DeviceGeometry}
   
-  \symdef[name=quasi-Fermi-potential]{FpOp}{\varphi_n}
-  \symdef[name=quasi-Fermi-potential]{Fp}[1]{\prefix\FpOp{#1}}
-  \symtest{Fp}{\Fp{x}}
+  \symdef[name=quasi-Fermi-potential]{QFPpOp}{\varphi_p}
+  \symdef[name=quasi-Fermi-potential]{QFPp}[1]{\prefix{\QFPpOp}{#1}}
+  \symtest{QFPp}{\QFPp{x}}
 \end{modsig}
 
 %%% Local Variables:

source/mmt/Quantities.mmt

@@ -52,7 +52,8 @@ theory SpatialDensity : qe:?SIUnits =
 theory SpatialPotential : qe:?SIUnits =
 	include Models/device?DeviceGeometry ❙
   /T Spatial variation of the potential,
-	   usually denoted by $φ$. ❙
+
+usually denoted by $φ$. ❙
 	potential : Ω → (QE ElectricPotential) ❘ # φ ❘ role Quantity ❙	
 ❚
 	
@@ -66,4 +67,4 @@ theory SpatialCurrentDensity : qe:?SIUnits =
    include Models/device?DeviceGeometry ❙
    include ?CurrentDensity ❙
 	spatialcurrentdensity : Ω → QE currentdensity_dim ❘ # j ❘ role Quantity ❙
-❚
\ No newline at end of file
+❚