Lesson 13 of 15

Higgs Mechanism

The Higgs Mechanism

The Higgs mechanism is the process by which the W and Z bosons — and all fundamental fermions — acquire mass without violating the gauge symmetries of the Standard Model. The discovery of the Higgs boson at CERN in 2012 (Nobel Prize 2013) confirmed this picture.

Spontaneous Symmetry Breaking and the VEV

The Higgs field ϕ\phi acquires a non-zero vacuum expectation value (VEV) vv at the minimum of its potential:

V(ϕ)=μ2ϕ2+λϕ4V(\phi) = -\mu^2|\phi|^2 + \lambda|\phi|^4

The VEV is fixed by the Fermi constant GFG_F:

v=12GF246.22 GeVv = \frac{1}{\sqrt{\sqrt{2}\, G_F}} \approx 246.22 \text{ GeV}

where GF=1.1663788×105G_F = 1.1663788 \times 10^{-5} GeV2^{-2}.

Gauge Boson Masses

Expanding around the VEV gives mass terms for the W and Z bosons. The W boson trilinear coupling to the Higgs is:

gHWW=2mW2vg_{HWW} = \frac{2 m_W^2}{v}

Similarly for the Z: gHZZ=2mZ2/vg_{HZZ} = 2m_Z^2/v.

Yukawa Couplings and Fermion Masses

Fermions couple to the Higgs field through Yukawa interactions:

LY=yfψˉfϕψf\mathcal{L}_Y = -y_f \bar{\psi}_f \phi \psi_f

After symmetry breaking, the fermion mass is mf=yfv/2m_f = y_f v / \sqrt{2}, so:

yf=2mfvy_f = \frac{\sqrt{2}\, m_f}{v}

The top quark (mt173m_t \approx 173 GeV) has yt1y_t \approx 1 — it is nearly as strongly coupled to the Higgs as theoretically natural. The electron (me0.511m_e \approx 0.511 MeV) has ye3×106y_e \approx 3 \times 10^{-6}, an unexplained hierarchy.

Your Task

Implement:

  • higgs_vev() — the Higgs VEV in GeV from GFG_F
  • yukawa_coupling(m_fermion_GeV) — Yukawa coupling yf=2mf/vy_f = \sqrt{2}\,m_f/v (compute vv inline)
  • higgs_to_WW_coupling(m_W_GeV) — trilinear Higgs–WW coupling 2mW2/v2m_W^2/v (compute vv inline)

All constants must be defined inside each function body.

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