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where ''q'' is the breakup momentum of the daughter particles and ''q<sub>0</sub>'' is the same, evaluated at ''m<sub>0</sub>''.
 
where ''q'' is the breakup momentum of the daughter particles and ''q<sub>0</sub>'' is the same, evaluated at ''m<sub>0</sub>''.
   −
The total expression becomes:
+
The final expression for the measured cross section becomes:
 +
:<math>
 +
\frac{d^8\sigma}{d\Omega_{b1}\,d\Omega_\omega\,d\Omega_\rho\,d\Omega_\pi} =
 +
\frac{1}{\sqrt{s}k_i}|T_{fi}|^2
 +
 
 +
\langle \Omega_\pi 0 0; \Omega_\rho \lambda_rho 0; \Omega_\omega \lambda_\omega 0; \Omega_{b1} \lambda_{b1} 0
 +
| U | \epsilon_\gamma; J_R \lambda_R \epsilon_R \rangle
    
:<math>
 
:<math>

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