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J_R \lambda_R \epsilon_R ; t, s; \Omega_0 \rangle
 
J_R \lambda_R \epsilon_R ; t, s; \Omega_0 \rangle
 
</math>
 
</math>
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Note that we leave the sum over <math>L_X</math> outside the amplitude of interest. This is convenient in partial wave analysis so that the hypothesized L-states can be listed and summed explicitly.
    
The intensity would then require an incoherent summation of amplitudes with laboratory x and y polarization.
 
The intensity would then require an incoherent summation of amplitudes with laboratory x and y polarization.
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