Representation Functions for the Degenerate Baryon Series in U(6)⊗U(6)
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The most degenerate class of representation functions dW,W′NB(θ) pertaining to U(6)⊗U(6) have been calculated for arbitrary quark number N with the baryon number B, and W, W′ weights of the U(6)W subgroup assuming the following values: B = 0, ⅓, ⅔, 1; [W], [W′] = 1, 6, 21, 56. These functions are the matrix elements of the rotation operator exp (−iΘJ2) between basis vectors of the degenerate U(6)⊗U(6) Feynman series (characterized entirely by BNW labels), and are essential to the generalized Reggeization program.
[1] M. Gell-Mann,et al. Series of hadron energy levels as representations of non-compact groups☆ , 1965 .
[2] G. C. Wick,et al. On the general theory of collisions for particles with spin , 1959 .
[3] R. Delbourgo,et al. REGGEIZATION OF U(6) x U(6). , 1968 .