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Line 114:
Line 114: − + − − :<math> − \frac{1}{\sqrt{2}} − \langle J m \epsilon|V| − \sqrt{-\epsilon_\gamma} \left( e^{-i\alpha}\left|1\; -1\right\rangle + − \epsilon_\gamma e^{i\alpha}\left|1\; +1\right\rangle \right) ; − J_R \lambda_R \epsilon_R ; t, s; \Omega_0 \rangle − </math> − which vanishes unless <math>\epsilon=\epsilon_\gamma\epsilon_R</math>, following from parity conservation.
Amplitudes for the Exotic b1π Decay (view source)
Revision as of 16:30, 15 August 2011
, 16:30, 15 August 2011→Photon-Reggeon-Resonance vertex
</math>
</math>
where <math>\alpha=\phi</math>, the azimuthal angle of the production plane in the lab system. Thus, the production amplitude becomes:
where <math>\alpha=\phi</math>, the azimuthal angle of the production plane in the lab system.
== Decay of t-channel resonance X to b1π==
== Decay of t-channel resonance X to b1π==