Particle Physics - Experimental Methods and Colliders
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1), and b(E) is the sum of e+ e− pair production, bremsstrahlung, and photonuclear contributions. 37) x0 ≈ (1/b) ln(1 + E0 /Eµc ) , where Eµc = a/b. 20 shows contributions to b(E) for iron. 002 GeV g−1 cm2 , b(E)E dominates the energy loss above several hundred GeV, where b(E) is nearly constant. The rates of energy loss for muons in hydrogen, uranium, and iron are shown in Fig. 21 . 20: Contributions to the fractional energy loss by muons in iron due to e+ e− pair production, bremsstrahlung, and photonuclear interactions, as obtained from Groom et al.
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