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(3) Interaction of high energy photons with matter - LUTH

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Compton scattering - <strong>energy</strong> transfer (1)<br />

What is the change in wavelength <strong>of</strong> a photon scattering <strong>of</strong>f an electron ?<br />

We describe the collision <strong>with</strong> relativistic 4-vectors:<br />

electron:<br />

photon:<br />

4-momentum conservation yields:<br />

p = [ me c , me v] p ' = [ ' mec , ' m<br />

<br />

e v ' ]<br />

[<br />

ℏ <br />

k =<br />

c<br />

, ℏ k] i c<br />

k' [<br />

ℏ '<br />

=<br />

c<br />

pk = p ' k '<br />

Scalar products <strong>of</strong> 4-vectors are Lorentz invariant:<br />

In the same way: p ' ⋅p ' = m e<br />

Thus:<br />

, ℏ ' '] ik c<br />

p ⋅p = 2 2 2 2 2 2 2 c<br />

me c − me v = me<br />

2 −v 2<br />

2<br />

v<br />

1−<br />

c 2<br />

= me 2 c 2 ; k⋅k = k ' ⋅k ' = 0<br />

pk 2 = p ' k ' 2<br />

p⋅p2p⋅kk⋅k = p ' ⋅p ' 2p ' ⋅k ' k ' ⋅k '<br />

p⋅k = p ' ⋅k '<br />

2 c 2<br />

A. Zech, Instrumentation in High Energy Astrophysics<br />

10

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