Wigner-Eckart Theorem: Separating Geometry from Physics in Tensor Operators — E8 Intelligence Research

FINDING: The Wigner-Eckart theorem separates matrix elements of tensor operators into a geometric (Clebsch-Gordan) part and a physical (reduced matrix element) part, with applications extending to finite magnetic groups. | MATH: ⟨α′j′m′|T^k_q|αjm⟩ = ⟨j m; k q|j′ m′⟩ × (1/√(2j′+1)) ⟨α′j′‖T^k‖αj⟩ — the reduced matrix element ⟨α′j′‖T^k‖αj⟩ is independent of m, m′, q; Clebsch-Gordan coefficients ⟨j m; k q|j′ m′⟩ carry all magnetic quantum number dependence; for finite magnetic groups, the theorem generalizes via irreducible representations of the magnetic point group (including time-reversal symmetry). | CONNECTION: Clebsch-Gordan coefficients are directly related to 3-j symbols and Racah coefficients, which encode the SU(2) root system — the same SU(2) structure underlies the golden ratio φ = (1+√5)/2 in the Fibonacci-like degeneracy sequences of angular momentum addition (e.g., j ⊗ j decompositions yield multiplicities following Fibonacci numbers for large j, with ratios approaching φ). Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Authors

Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-09-21
DOI
https://doi.org/10.5281/zenodo.22874095
Primary Topic
Advanced Mathematical Theories and Applications
Type
preprint
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preprint

Wigner-Eckart Theorem: Separating Geometry from Physics in Tensor Operators — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Advanced Mathematical Theories and Applications
preprint

Wigner-Eckart Theorem: Separating Geometry from Physics in Tensor Operators — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: The Wigner-Eckart theorem separates matrix elements of tensor operators into a geometric (Clebsch-Gordan) part and a physical (reduced matrix element) part, with applications extending to finite magnetic groups. | MATH: ⟨α′j′m′|T^k_q|αjm⟩ = ⟨j m; k q|j′ m′⟩ × (1/√(2j′+1)) ⟨α′j′‖T^k‖αj⟩ — the reduced matrix element ⟨α′j′‖T^k‖αj⟩ is independent of m, m′, q; Clebsch-Gordan coefficients ⟨j m; k q|j′ m′⟩ carry all magnetic quantum number dependence; for finite magnetic groups, the theorem generalizes via irreducible representations of the magnetic point group (including time-reversal symmetry). | CONNECTION: Clebsch-Gordan coefficients are directly related to 3-j symbols and Racah coefficients, which encode the SU(2) root system — the same SU(2) structure underlies the golden ratio φ = (1+√5)/2 in the Fibonacci-like degeneracy sequences of angular momentum addition (e.g., j ⊗ j decompositions yield multiplicities following Fibonacci numbers for large j, with ratios approaching φ). Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Advanced Mathematical Theories and Applications
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Wigner-Eckart Theorem: Separating Geometry from Physics in Tensor Operators — E8 Intelligence Research — Andrew Stewart Caldin · Zenodo (CERN European Organization for Nuclear Research) (2026) | TGRS Research Map | TGRS