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Amplitudes for the Exotic b1π Decay (view source)
Revision as of 22:31, 15 August 2011
, 22:31, 15 August 2011→Assembly of the full amplitude
\frac{d^8\sigma}{d\Omega_{b1}\,d\Omega_\omega\,d\Omega_\rho\,d\Omega_\pi} =
\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
\frac{1}{\sqrt{s}k_i}|T_{fi}|^2
\left(\frac{q_{b1}}{16\pi^2}\right)
\left(\frac{q_{\omega}}{16\pi^2}\right)
\left(\frac{q_{\rho}}{16\pi^2}\right)
\left(\frac{q_{\pi}}{16\pi^2}\right)
</math>
</math>
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