Suppose the hypercharges of one generation were not known

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Particle Physics & Quantum Fields · Beyond the Standard Model

Symmetry and Flavour, Ch Grand unification: running couplings, SU(5), proton decay and the hierarchy problem

Problem

Suppose the hypercharges of one generation were not known. Keep the fields and their SU(3)×SU(2)SU(3)\times SU(2) content, Q (3,2)Q\,(3,2), uc (3ˉ,1)u^c\,(\bar3,1), dc (3ˉ,1)d^c\,(\bar3,1), L (1,2)L\,(1,2) and ec (1,1)e^c\,(1,1), but give them unknown hypercharges yQy_Q, yuy_u, ydy_d, yLy_L and yey_e, with yQ≠0y_Q\neq0. Require the four anomaly sums of this chapter to vanish: the mixed sum over the colour triplets and antitriplets, the mixed sum over the weak doublets, ∑Y=0\sum Y=0 and ∑Y3=0\sum Y^3=0, each state counted with its multiplicity. ((a)) Write the two mixed sums and show that they give yu+yd=−2yQy_u+y_d=-2y_Q and yL=−3yQy_L=-3y_Q. ((b)) Use ∑Y=0\sum Y=0 to find yey_e in terms of yQy_Q. ((c)) Use ∑Y3=0\sum Y^3=0 to show that yuy_u and ydy_d are −4yQ-4y_Q and 2yQ2y_Q in some order. Calling ucu^c the field with hypercharge −4yQ-4y_Q and taking yQ=16y_Q=\tfrac16, find yLy_L, yey_e, yuy_u and ydy_d. ((d)) Show that, for any yQy_Q, the hypercharges of dcd^c and LL satisfy 3yd+2yL=03y_d+2y_L=0, the tracelessness of hypercharge on the 5ˉ\bar5 that SU(5)SU(5) requires.

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