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CERN Program Library Long Writeup W5013 - CERNLIB ...

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Much of the difficulty in approximating multiple Coulomb scattering in terms of the radiation length is that<br />

the number of radiation lengths is a poor measure of the scattering. A better expression, which is used in<br />

GEANT has been proposed by [42]:<br />

θ 2 0 =<br />

[ ]<br />

χ2 c 1+ν<br />

1+F 2 log(1 + ν) − 1<br />

ν<br />

(3)<br />

where<br />

ν =<br />

Ω 0<br />

2(1 − F )<br />

F = fraction of the tracks in the sample<br />

Ω 0 =<br />

χ 2 c<br />

1.167χ 2 α<br />

is the mean number of scatters<br />

χ 2 c and χ 2 α are parameters of the Molière theory, for which the reader is invited to see [PHYS325], and<br />

1.167 ≈ exp(2γ − 1) where γ is the Euler’s constant =0.57721 .... This form, which is the result of<br />

empirical fits, is derived from the screened Rutherford cross section, which has the form 2χ 2 α/(χ 2 α + θ0 2).<br />

For F anywhere from 0.9 to 0.995 this expression represents Molière scattering to better than 2% for 10 <<br />

Ω 0 < 10 8 , which covers singly charged relativistic particles (β ≈ 1) in the range 10 −3

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