A. Zee, Quantum Field Theory in a Nutshell · Problem IV.6.2

Field Theory Redux

Physics — QFT

Problem

In general, there may be several Higgs fields belonging to various representations labeled by α\alpha. Show that the mass squared matrix for the gauge bosons generalize immediately to (μ2)ab=∑αg2(Tαavα⋅Tαbvα)(\mu^2)_{ab} = \sum_\alpha g^2(T^a_\alpha v_\alpha \cdot T^b_\alpha v_\alpha), where vαv_\alpha is the vacuum expectation value of ϕα\phi_\alpha and TαaT^a_\alpha is the aath generator represented on ϕα\phi_\alpha. Apply this to the situations described in exercises IV.6.1 and IV.6.2 and work out the mass spectrum of the gauge bosons.

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