Changes

| [[Image:hVb702_T25.gif|250px]] || [[Image:hVb710_T25.gif|250px]]

| [[Image:hVb702_T25.gif|250px]] || [[Image:hVb710_T25.gif|250px]]

|-

|-

|colspan="2" | Pulse height spectrum at fixed pulser intensity and temperature 25°C, and increasing bias voltage V_b = 69.5V (upper left), 70.0V (upper right), 70.2V (lower left), and 71.0V (lower right).

<|colspan="2" | Pulse height spectrum at fixed pulser intensity and temperature 25&deg;C, and increasing bias voltage V_b = 69.5V (upper left), 70.0V (upper right), 70.2V (lower left), and 71.0V (lower right).

|-

|-

|}

|}

* The Gaussian smearing of the individual pixel pulse-height distribution was replaced with the following function that has an asymmetric tail.

* The Gaussian smearing of the individual pixel pulse-height distribution was replaced with the following function that has an asymmetric tail.

::<math>

::<math>

f(x;\alpha,\beta,\sigma) = \beta\frac{\alpha}{2}\,e^{\alpha x+\frac{\alpha^2\sigma^2}{2}}\left[1-Erf\left(\frac{x+\alpha\sigma^2}{\sqrt{2}\sigma}\right)\right] <br>:: + \frac{1-\beta}{\sqrt{2\pi}\sigma}e^{-\frac{x^2}{2\sigma^2}}\\

f(x;\alpha,\beta,\sigma) = \beta\frac{\alpha}{2}\,e^{\alpha x+\frac{\alpha^2\sigma^2}{2}}\left[1-Erf\left(\frac{x+\alpha\sigma^2}{\sqrt{2}\sigma}\right)\right] </math><br>

:: <math> + \frac{1-\beta}{\sqrt{2\pi}\sigma}e^{-\frac{x^2}{2\sigma^2}}\\

\end{eqnarray}}</math>

\end{eqnarray}}</math>

: This function is normalized to unity and is described by two parameters:

: This function is normalized to unity and is described by two parameters: