Diamond Detectors for Ionizing Radiation - HEPHY
Diamond Detectors for Ionizing Radiation - HEPHY
Diamond Detectors for Ionizing Radiation - HEPHY
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Chapter 4<br />
Solid State Detector Theory<br />
When a heavy charged particle traverses material, energy is mainly transfered due to<br />
Coulomb interactions between the particle and the atomic electrons in the material. In<br />
solids with an atomic lattice, which can be described by the band model, the electrons<br />
are excited from the valence to the conduction band when the particle transfers enough<br />
energy. This process is known as electron-hole generation. At very high incident particle<br />
energies, also radiation is emitted when collisions occur, which is called bremsstrahlung.<br />
4.1 Bethe-Bloch Theory<br />
H.A. Bethe 1 and F. Bloch 2 developed a theory based on energy and momentum<br />
conservation <strong>for</strong> the energy loss of charged particles other than electrons at high energies<br />
(v c) traversing material, stated in terms of dE=dx, when radiative energy loss is<br />
negligible [13, 14].<br />
"<br />
, 1 dE<br />
dx =4N Ar 2 e m ec 2 z 2Z 1 1<br />
A 2 2 ln 2m ec 2 2 2 T max<br />
! #<br />
, 2 , () (4.1)<br />
I 2<br />
2<br />
Eq. 4.1 represents the dierential energy loss per mass surface density [MeV (g cm ,2 ) ,1 ],<br />
where ze is the charge of the incident particle, N A , Z and A are Avogadro's number, the<br />
atomic number and the atomic mass of the material, m e and r e are the electron mass and<br />
e<br />
its classical radius (<br />
2<br />
4 0 m ec<br />
). T 2 max is the maximum kinetic energy which is still detected<br />
in the material, I is the mean excitation energy, = v=c, = (1 , 2 ) ,1=2 and () is<br />
a correction <strong>for</strong> the shielding of the particle's electric eld by the atomic electrons, the<br />
density eect caused by atomic polarization.<br />
For 0:1 < < 1:0, the dE=dx curves (g. 4.1) approximately fall proportionally to<br />
,2 , then show a broad minimum at =3to 4 (decreasing with Z) and nally slowly<br />
1 Hans Albrecht Bethe, *1906 in Strasbourg. Most of the time he worked with the Cornell University,<br />
interrupted by sabbaticals leading him to CERN and other research centers. For his contributions<br />
to the theory of nuclear reactions he was awarded the Nobel Prize in 1967.<br />
2 Felix Bloch, *1905 in Zurich, y1983. He was working with a number of universities and research<br />
centers, like Stan<strong>for</strong>d and CERN. The Nobel Prize was awarded to him in 1952 <strong>for</strong> nuclear magnetic<br />
precision measurements.<br />
15