A. Zee, Quantum Field Theory in a Nutshell · Problem VII.2.1

Field Theory Redux

Physics — QFT

Problem

Unfortunately, the mass of the elusive Higgs particle HH depends on the parameters in the double well potential V=−μ2ϕ†ϕ+λ(ϕ†ϕ)2V = -\mu^2\phi^\dagger\phi + \lambda(\phi^\dagger\phi)^2 responsible for the spontaneous symmetry breaking. Assuming that HH is massive enough to decay into W++W−W^+ + W^- and Z+ZZ + Z, determine the rates for HH to decay into these modes.

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