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Line 198:
Line 198: − + − \begin{array}{c} − \scriptstyle{R,\lambda_R}\\ − \vspace*{-10pt} − \scriptstyle{\lambda_{b_1},\lambda_\omega,\lambda_\rho} − \end{array}}
Amplitudes for the Exotic b1π Decay (view source)
Revision as of 19:38, 15 August 2011
, 19:38, 15 August 2011→Assembly of the full amplitude
where the T matrix element contains a sum over all intermediate states that contribute to the process. In terms of the individual decay matrix elements introduced earlier, the T matrix element can be written as
where the T matrix element contains a sum over all intermediate states that contribute to the process. In terms of the individual decay matrix elements introduced earlier, the T matrix element can be written as
:<math>
:<math>
T_{fi} = \sum_{
T_{fi} = \sum_{R,\lambda_R}\lambda_{b_1},\lambda_\omega,\lambda_\rho}
\langle \Omega_\pi 0 0; \Omega_\rho \lambda_\rho 0; \Omega_\omega \lambda_\omega 0; \Omega_{b1} \lambda_{b1} 0
\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
| U | \epsilon_\gamma; J_R \lambda_R \epsilon_R \rangle