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Clebsch–Gordan Coefficients: Orthogonality, Recursion, and Lattice QCD Applications — E8 Intelligence Research

  1. 1Independent Researcher, United Kingdom

Abstract

FINDING: Search results are pedagogical resources on Clebsch–Gordan (CG) coefficients, with one lattice-QCD application paper; no explicit proof of golden-ratio absence is found in the returned material. | MATH: CG coefficients ⟨j₁ m₁; j₂ m₂ | J M⟩ are the overlap matrix elements between uncoupled and coupled angular-momentum bases; they satisfy orthogonality ∑_{m₁,m₂} ⟨j₁m₁;j₂m₂|JM⟩⟨j₁m₁;j₂m₂|J′M′⟩ = δ_{JJ′}δ_{MM′}, and recursion relations from ladder operators. The lattice paper uses double-valued irreps of the octahedral group (O_h^D), whose dimensions are {1,2,3,4} — no φ appears. | CONNECTION: CG coefficients for SU(2) are algebraic numbers from square roots of rationals (e.g., √(2/3), √(1/2)); the golden ratio φ = (1+√5)/2 is quadratic irrational but not of the form √(p/q) with p,q integers unless p/q = φ² — which is impossible since φ² is irrational. Thus φ cannot appear as a CG coefficient magnitude. However, φ *can* appear in SU(3) or higher-rank tensor products via ratios of

Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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BibTeX
@misc{caldin2026clebschgordan,
  title = {{Clebsch–Gordan Coefficients: Orthogonality, Recursion, and Lattice QCD Applications — E8 Intelligence Research}},
  author = {Andrew Stewart Caldin},
  howpublished = {Zenodo},
  year = {2026},
  month = oct,
  doi = {10.5281/zenodo.23587358},
  url = {https://zenodo.org/records/23587358},
  note = {CC BY 4.0},
}
RIS
TY  - UNPB
TI  - Clebsch–Gordan Coefficients: Orthogonality, Recursion, and Lattice QCD Applications — E8 Intelligence Research
AU  - Andrew Stewart Caldin
PY  - 2026
DA  - 2026/10/23
PB  - Zenodo
DO  - 10.5281/zenodo.23587358
UR  - https://zenodo.org/records/23587358
AB  - FINDING: Search results are pedagogical resources on Clebsch–Gordan (CG) coefficients, with one lattice-QCD application paper; no explicit proof of golden-ratio absence is found in the returned material. | MATH: CG coefficients ⟨j₁ m₁; j₂ m₂ | J M⟩ are the overlap matrix elements between uncoupled and coupled angular-momentum bases; they satisfy orthogonality ∑_{m₁,m₂} ⟨j₁m₁;j₂m₂|JM⟩⟨j₁m₁;j₂m₂|J′M′⟩ = δ_{JJ′}δ_{MM′}, and recursion relations from ladder operators. The lattice paper uses double-valued irreps of the octahedral group (O_h^D), whose dimensions are {1,2,3,4} — no φ appears. | CONNECTION: CG coefficients for SU(2) are algebraic numbers from square roots of rationals (e.g., √(2/3), √(1/2)); the golden ratio φ = (1+√5)/2 is quadratic irrational but not of the form √(p/q) with p,q integers unless p/q = φ² — which is impossible since φ² is irrational. Thus φ cannot appear as a CG coefficient magnitude. However, φ *can* appear in SU(3) or higher-rank tensor products via ratios of  Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
ER  -