← Quantum Field Theory
Topic 15 of 22
Spontaneous Symmetry Breaking
A Lagrangian can be symmetric while the ground state is not. When the vacuum spontaneously selects a direction in field space, the symmetry is broken without any explicit breaking term. Goldstone's theorem then guarantees one massless scalar — a Nambu-Goldstone boson — per broken symmetry generator. This underlies the pseudo-Goldstone pions of QCD and (with a gauge-theory twist) the mass generation of W and Z.
Key Concepts
- Order parameter ⟨φ⟩ = v ≠ 0 selects a vacuum that breaks the symmetry of the Lagrangian
- Mexican hat potential: V = −μ²|φ|² + λ|φ|⁴, minimum at |φ| = v = √(μ²/2λ)
- Goldstone's theorem: one massless scalar per broken generator (dim G − dim H)
- Massive mode (Higgs-like): oscillation in radial direction, mH = √(2μ²)
- Massless Goldstone: oscillation along flat angular direction, no restoring force
- Pseudo-Goldstone bosons: explicit breaking makes them light but not massless (e.g., pions, mπ ≪ mρ)
Key Equations
Mexican hat potential
Field decomposition
Goldstone counting
Pion EFT
Worked Example
Example Problem
Problem
For V = −μ²|φ|²+λ|φ|⁴ with μ = 100 GeV, λ = 0.5, find v and mh.
Solution
v = √(μ²/2λ) = √(10000/1) = 100 GeV. The Higgs mass comes from V″ at the minimum: V″(v) = −2μ²+12λv² = −20000+60000 = 40000, so mh = √40000 = 200 GeV = 2μ.
Key Takeaways
- SSB: the Lagrangian has symmetry G but the vacuum ⟨φ⟩=v breaks G → H; physics observes the broken symmetry
- Goldstone's theorem: N_GB = dim G − dim H massless scalars must appear in the spectrum for each broken continuous symmetry generator
- Radial (Higgs-like) mode is massive (mh = √(2λ)v); angular (Goldstone) mode is exactly massless if the symmetry is exact
- Pions are pseudo-Goldstone bosons of approximate chiral symmetry of QCD, explaining why mπ ≪ mρ ≈ 770 MeV