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Quantum Field Theory. Note « 13 »

Spontaneous symmetry breaking. Higgs mechanism. (Moulders,chapter 12)
Goldstone theorem.
If a theory has a symmetry, such as SO(2) symmetry,
L = ½ (∂μσ∂μσ + ∂μπ∂μπ) - V(π22)
V(S) = ½ m2 S + λ S2
which is not the symmetry of the ground state (vacuum)
m2 < 0 , λ > 0 ⇒ S0 = - m2/ ≠ 0
then the theory will have a massive particle and a massless particle.
Higgs mechanism.
If the symmetry breaking happens in a gauge theory
L = ½ Dμφ Dμφ - V(φ2) - 1/4 GμνGμν
than a massive scalar particle appears, called Higgs boson, and some gauge bosons become massive.
Exercises
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