| 1 | % GEANT4 Physics Reference Manual - Scintillation Process
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| 2 | % in LaTex 2e - by P. Gumplinger
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| 3 |
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| 4 | %\documentclass[11pt,twoside,a4page]{article}
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| 5 | %\usepackage{epsfig}
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| 6 |
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| 7 | %\setlength{\parindent}{0pt}
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| 8 |
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| 9 | %\begin{document}
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| 10 |
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| 11 | %\title{Scintillation}
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| 12 | %\author{P.~Gumplinger}
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| 13 | %\date{December 7, 1998}
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| 14 | %\maketitle
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| 15 |
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| 16 | \section{Scintillation}
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| 17 |
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| 18 | Every scintillating material has a characteristic light yield, $Y\,
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| 19 | (photons/MeV$), and an intrinsic resolution which generally broadens
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| 20 | the statistical distribution, $\sigma_i/\sigma_s > 1$, due to impurities
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| 21 | which are typical for doped crystals like NaI(Tl) and CsI(Tl). The
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| 22 | average yield can have a non-linear dependence on the local energy
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| 23 | deposition. Scintillators also have a time distribution spectrum with
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| 24 | one or more exponential decay time constants, $\tau_{i}$, with each
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| 25 | decay component having its intrinsic photon emission spectrum. These are
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| 26 | empirical parameters typical for each material. \\
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| 27 |
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| 28 | \noindent
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| 29 | The generation of scintillation light can be simulated by sampling the
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| 30 | number of photons from a Poisson distribution. This distribution is based
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| 31 | on the energy lost during a step in a material and on the scintillation
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| 32 | properties of that material. The frequency of each photon is sampled from
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| 33 | the empirical spectra. The photons are generated evenly along the track
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| 34 | segment and are emitted uniformly into $4\pi$ with a random linear
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| 35 | polarization.
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| 36 |
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| 37 | \subsection{Status of this document}
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| 38 | 07.12.98 created by P.Gumplinger
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| 39 |
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| 40 | %\end{document}
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