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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

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