integrable-systems-physics

Layer 1 — Physics24 concepts in this subtree

Classical and quantum many-body systems with as many independent conservation laws as degrees of freedom, permitting exact solution by algebraic rather than perturbative methods. Classical: Liouville-Arnold theorem — N-DOF Hamiltonian…

XXX Heisenberg spin chain: Bethe-ansatz diagonalisation
KdV Lax pair: infinitely-many conservation laws via spectral invariance
Yang-Baxter equation + 6-vertex / 8-vertex models
XXX one-magnon dispersion E(k) = 2J(1 - cos k); ratio E(π)/E(π/3) = 4
KdV 1-soliton u = 2κ²·sech²(κ(x - 4κ²t)) satisfies u_t+6uu_x+u_xxx=0 exactly
6-vertex ice-rule anisotropy Δ = 1/2 (critical massless regime)
Lax-pair spectral curve: L*psi = lambda*psi defines Riemann surface C_g with dim Omega^1(C_g) = g
sl(2) quadratic Casimir C_2 = j(j+1); U_q(sl(2)) Hopf algebra structure (R-matrix via comultiplication)
Grassmannian Gr(2,4) Plücker relation: p_12*p_34 - p_13*p_24 + p_14*p_23 = 0 in P^5
Theorem: compact Riemann surface C_g has dim H^0(C_g, Omega^1) = g (algebraic-geometric invariant)
Theorem: sl(2) quadratic Casimir C_2 = j(j+1) evaluates to 3/4 at spin j = 1/2
Theorem: Gr(2,4) Plücker identity p_12*p_34 - p_13*p_24 + p_14*p_23 = 0 (algebraic identity in 2x4 matrix)
GGKM (1967)
KdV solitons (1965)
Bethe ansatz (1931)
Painleve property (1900)
Yang-Baxter (1967)
Lax pair (1968)
KdV soliton (Zabusky-Kruskal 1965)
Lax pair (Lax 1968)
Inverse scattering (GGKM 1967)
Yang-Baxter (1967)
Toda lattice (1967)
Painlevé (1900)
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