Manual: drop labels (d93468de) · Commits · XRFLab109 / Allpix Squared

doc/usermanual/05_models/05_impact_ionization.md

+0 −6

Original line number	Diff line number	Diff line
		@@ -14,7 +14,6 @@ configurable threshold $`E_{\textrm{thr}}`$, unity gain is assumed:

		```math
		\begin{equation}
		\label{eq:multiplication}
		g (E, T) = \left\{
		\begin{array}{ll}
		e^{l \cdot \alpha(E, T)} & E > E_{\textrm{thr}}\\
		@@ -33,7 +32,6 @@ The ionization coefficients are parametrized as

		```math
		\begin{equation}
		\label{eq:multi:massey}
		\alpha (E, T) = A e^{-\frac{B(T)}{E}},
		\end{equation}
		```
		@@ -76,7 +74,6 @@ The Van Overstraeten-De Man model \[[@overstraeten]\] describes impact ionizatio

		```math
		\begin{equation}
		\label{eq:multi:man}
		\alpha (E, T) = \gamma (T) \cdot a_{\infty} \cdot e^{-\frac{\gamma(T) \cdot b}{E}},
		\end{equation}
		```
		@@ -85,7 +82,6 @@ For holes, two sets of impact ionization parameters $`p = \left\{ a_{\infty}, b

		```math
		\begin{equation}
		\label{eq:multi:man:h}
		p = \left\{
		\begin{array}{ll}
		p_{\textrm{low}} & E < E_{0}\\
		@@ -135,7 +131,6 @@ features a linear dependence on the electric field strength $`E`$. The coefficie

		```math
		\begin{equation}
		\label{eq:multi:oku}
		\alpha (E, T) = a(T) \cdot E \cdot e^{-\left(\frac{b(T)}{E}\right)^2}.
		\end{equation}
		```
		@@ -182,7 +177,6 @@ coefficient takes a different form than the previous models and is given by

		```math
		\begin{equation}
		\label{eq:multi:bologna}
		\alpha (E, T) = \frac{E}{a(T) + b(T) e^{d(T) / \left(E + c(T) \right)}},
		\end{equation}
		```