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10 CHAPTER 1. INTRODUCTION<br />

− dE<br />

dx<br />

⏐<br />

⏐ col<br />

= ρ NA<br />

A<br />

<br />

Emax<br />

Emin<br />

′ dσ<br />

E<br />

dE ′<br />

⏐<br />

⏐ col<br />

dE ′ = ρ NA<br />

A kcol . (1.3)<br />

In literature one often finds the thickness dx measured in g/cm2 and the energy loss<br />

− dE<br />

⏐ given in MeV cm col 2 /g. We will note − 1<br />

⏐<br />

dE ⏐ instead, which leaves dx with<br />

col<br />

dx<br />

ρ dx<br />

the unit length. Let kcol(ν) the energy loss resulting from close collisions, then the total energy loss is<br />

given by the sum of the two<br />

Distant Collisions<br />

− 1 dE<br />

⏐<br />

ρ dx<br />

⏐ col<br />

= NA<br />

A<br />

<br />

kcol(ν) . (1.4)<br />

For the calculation of the energy loss due to distant collisions kcol(

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