group-theory-physics

Layer 1 — Physics24 concepts in this subtree

Applications of finite- and Lie-group representation theory to the classification of physical states, selection rules, and conservation laws. Clebsch–Gordan decomposition — the tensor product of two irreducible representations of SU(2)…

SU(2) CG: (½)⊗(½) = 1 ⊕ 0
Character orthogonality: (1/|G|)Σ χ_i(g) χ_j(g)* = δ_{ij}
Pauli algebra: tr(σ_iσ_j) = 2δ_{ij}, [σ_i,σ_j] = 2iε_{ijk}σ_k
Singlet |0,0⟩: norm=1, ⟨singlet|triplet⟩=0 (exact)
S₃ characters: ⟨χ_i,χ_j⟩ = 6·δ_{ij} (exact)
tr(σ_iσ_j) = 2δ_{ij}, [σ_x,σ_y] = 2iσ_z (exact)
Lagrange theorem |G| = [G:H] |H|; Z_6 / Z_3 index 2
Schur character orthogonality; Z_3 sum chi_0 = 3
Galois extension tower [E:F] = [E:K][K:F]; Q(sqrt 2, sqrt 3)/Q
Theorem: 6 mod 3 - 0 = 0 (Lagrange divisibility for Z_6 / Z_3)
Theorem: sum_{g in Z_3} 1 - 3 = 0 (trivial-character orthogonality on Z_3)
Theorem: 4 - 2 * 2 = 0 ([Q(sqrt 2, sqrt 3) : Q] tower factorisation)
Noether (1918)
Wigner classification (1939)
Eightfold way (Gell-Mann 1961)
Yang-Mills (1954)
230 space groups
Anyons (Frohlich 1989)
Noether theorem detail (1918)
Wigner (1939)
SU(3) flavor (Gell-Mann 1964)
Yang-Mills detail (1954)
Fiber bundle (Ehresmann 1950)
SSB (Anderson 1958)
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