Spontaneous Symmetry Breaking Modifies Wigner–Eckart Selection Rules via Goldstone Modes — E8 Intelligence Research

FINDING: Spontaneous symmetry breaking (SSB) modifies Wigner–Eckart matrix-element selection rules via Goldstone-mode contributions, with corrections scaling as inverse powers of the order parameter (arXiv:2007.03539). MATH: - Wigner–Eckart (unbroken): ⟨j' m'| T^(k)_q |j m⟩ = ⟨j m; k q | j' m'⟩ · ⟨j'||T^(k)||j⟩ / √(2j'+1). All m-dependence isolated in one Clebsch–Gordan coefficient; the reduced matrix element ⟨j'||T^(k)||j⟩ is m-independent. - SSB correction (infinite-volume, G → H): ⟨j' m'| T^(k)_q |j m⟩ = [CG]·⟨j'||T^(k)||j⟩ + Σ_α (Goldstone-pole terms) ∝ 1/⟨φ⟩^n, where ⟨φ⟩ is the vacuum expectation value (order parameter) and the extra terms arise from the broken generators' Nambu–Goldstone modes. - Goldstone theorem: one massless boson per broken generator; #NG = dim(G) − dim(H). Dispersion ω(k) → 0 as k → 0. - Higgs mechanism (gauge case): NG modes are "eaten," giving M_A = g⟨φ⟩; the would-be Goldstone becomes the longitudinal polarization. - Clebsch–Gordan / SU(2) recoupling: j₁ Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-10-27
DOI
https://doi.org/10.5281/zenodo.23684975
Primary Topic
Particle physics theoretical and experimental studies
Type
preprint
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Spontaneous Symmetry Breaking Modifies Wigner–Eckart Selection Rules via Goldstone Modes — E8 Intelligence Research

Andrew Stewart Caldin
13 links
Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
preprint

Spontaneous Symmetry Breaking Modifies Wigner–Eckart Selection Rules via Goldstone Modes — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Spontaneous symmetry breaking (SSB) modifies Wigner–Eckart matrix-element selection rules via Goldstone-mode contributions, with corrections scaling as inverse powers of the order parameter (arXiv:2007.03539). MATH: - Wigner–Eckart (unbroken): ⟨j' m'| T^(k)_q |j m⟩ = ⟨j m; k q | j' m'⟩ · ⟨j'||T^(k)||j⟩ / √(2j'+1). All m-dependence isolated in one Clebsch–Gordan coefficient; the reduced matrix element ⟨j'||T^(k)||j⟩ is m-independent. - SSB correction (infinite-volume, G → H): ⟨j' m'| T^(k)_q |j m⟩ = [CG]·⟨j'||T^(k)||j⟩ + Σ_α (Goldstone-pole terms) ∝ 1/⟨φ⟩^n, where ⟨φ⟩ is the vacuum expectation value (order parameter) and the extra terms arise from the broken generators' Nambu–Goldstone modes. - Goldstone theorem: one massless boson per broken generator; #NG = dim(G) − dim(H). Dispersion ω(k) → 0 as k → 0. - Higgs mechanism (gauge case): NG modes are "eaten," giving M_A = g⟨φ⟩; the would-be Goldstone becomes the longitudinal polarization. - Clebsch–Gordan / SU(2) recoupling: j₁ Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Particle physics theoretical and experimental studies
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