as taken from equations~1 (for electrons) and~4 (for holes) of~\cite{masetti}.
Only the parameters $\mu_{max}$ for both electrons and holes are temperature dependent and are scaled according to Equation~\eqref{eq:mob:ham:temp} with parameters $\gamma_e =-2.5$ for electrons and $\gamma_h =-2.2$ for holes.
The parameter values implemented in \apsq are taken from Table~I of~\cite{masetti} as:
The parameter values implemented in \apsq are taken from Table~I of~\cite{masetti}for phosphorus and boron as:
\begin{equation*}
\begin{split}
\mu_{0,e}&= \SI{52.2}{cm^2 \per V \per s}\\
\mu_{max,e}&= \SI{1417}{cm^2 \per V \per s}\cdot (T / \SI{300}{K})^{-2.5}\\
C_{r,e}&= \SI{9.68e16}{\per\cubic\cm}\\
\alpha_{e}&= 0.68\\
\mu_{1,e}&= \SI{43.4}{cm^2 \per V \per s}\\
C_{s,e}&= \SI{3.43e20}{\per\cubic\cm}\\
\beta_{e}&= 2.0\\
\mu_{0,e}&= \SI{68.5}{cm^2 \per V \per s}\\
\mu_{max,e}&= \SI{1414}{cm^2 \per V \per s}\cdot (T / \SI{300}{K})^{-2.5}\\
C_{r,e}&= \SI{9.20e16}{\per\cubic\cm}\\
\alpha_{e}&= 0.711\\
\mu_{1,e}&= \SI{56.1}{cm^2 \per V \per s}\\
C_{s,e}&= \SI{3.41e20}{\per\cubic\cm}\\
\beta_{e}&= 1.98\\
\end{split}
\qquad
\begin{split}
@@ -187,10 +187,10 @@ The mobility is parametrized as
as taken from equations~8 (for electrons) and~12 (for holes) of~\cite{arora}.
as taken from equations~8 (for electrons) and~13 (for holes) of~\cite{arora}.
The parameter values are provided at the reference temperature of \SI{300}{K} and scaled to different temperatures according to Equation~\eqref{eq:mob:ham:temp}.
The values implemented in \apsq are taken from Table~1 of~\cite{arora} as:
The values implemented in \apsq are taken from Table~1 and the formulas of~\cite{arora} as:
\begin{equation*}
\begin{split}
\mu_{min,e}&= \SI{88.0}{cm^2 \per V \per s}\cdot (T / \SI{300}{K})^{-0.57}\\