@@ -399,6 +399,7 @@ While~\cite{kramberger} quotes different values for $\beta$ for irradiation with
The parameters arise from measurements of the were obtained evaluating current signals of irradiated sensors via light injection at fluences up to $\Phi_{eq}=\SI{2e14}{n_{eq}\per\cm^2}$.
This model can be selected in the configuration file via the parameter \parameter{trapping_model = "ljubljana"}.
\subsection{Dortmund}
@@ -424,6 +425,8 @@ The values have been extracted evaluating current signals of irradiated sensors
No temperature scaling is provided.
Values for neutron and proton irradiation have been evaluated in~\cite{dortmundTrapping}, \apsq makes use of the values for proton irradiation.
This model can be selected in the configuration file via the parameter \parameter{trapping_model = "dortmund"}.
\subsection{CMS Tracker}
This effective trapping model has been developed by the CMS Tracker Group.
@@ -448,6 +451,8 @@ The interpolation of the results follows the relation
No temperature scaling is provided.
This model can be selected in the configuration file via the parameter \parameter{trapping_model = "cmstracker"}.
\subsection{Mandic}
The Mandi\'{c} model~\cite{Mandic} is an empirical model developed from measurements with high fluences ranging from $\Phi_{eq}=\SI{5e15}{n_{eq}\per\cm^2}$ to $\Phi_{eq}=\SI{1e17}{n_{eq}\per\cm^2}$ and describes the lifetime via
@@ -473,7 +478,7 @@ with the parameters
The parameters for electrons are taken from~\cite{Mandic}, for measurements at a temperature of $\SI{-20}{\celsius}$, and the results extrapolated to $\SI{-30}{\celsius}$.
A scaling from electrons to holes was performed based on the default values in Weightfield2~\cite{Weightfield2}.
\cite{Mandic}
This model can be selected in the configuration file via the parameter \parameter{trapping_model = "mandic"}.
