Changes

\frac{1}{\sqrt{s}k_i}|T_{fi}|^2

\frac{1}{\sqrt{s}k_i}|T_{fi}|^2

</math>

</math>

where the T matrix element contains a sum over all intermediate states that contribute to the process.  Here the proton target and recoil are treated as a virtual beam of Reggeons in a virtual collider experiment.

where the T matrix element contains a sum over all intermediate states that contribute to the process.  Here the proton target and recoil are treated as a virtual beam of Reggeons in a virtual collider experiment. In terms of the individual decay matrix elements introduced earlier, the T matrix element can be written as

:<math>

:<math>

\langle \Omega_\pi 0 0; \Omega_\rho \lambda_rho 0; \Omega_\omega \lambda_\omega 0; \Omega_{b1} \lambda_{b1} 0

T_{fi} = \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

</math>

</math>