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4.1. Classical particle kinematics
Figure 4.2: Initial and final states, CM frame.
Figure 4.3: Initial and final states, lab frame.
tering angles θ 1 and θ 2 in the lab frame in terms of the scattering
angle θ
� in the CM frame. This is accomplished in principle by
Lorentz transformation from the CM to lab frame as follows:
q 1z = γ (q 1
�
z + β ε
�
1 )
4.1. Classical particle kinematics
Figure 4.2: Initial and final states, CM frame.
Figure 4.3: Initial and final states, lab frame.
tering angles θ 1 and θ 2 in the lab frame in terms of the scattering
angle θ
� in the CM frame. This is accomplished in principle by
Lorentz transformation from the CM to lab frame as follows:
q 1z = γ (q 1
�
z + β ε
�
1 )