conformal-field-theory

Layer 1 — Physics24 concepts in this subtree

Quantum field theories invariant under the conformal group — in 2D, the infinite-dimensional Virasoro algebra — governing critical phenomena, worldsheet string theories, and exact-solvable lattice models. Virasoro algebra — the Laurent…

Virasoro: [L_m,L_n] = (m−n)L_{m+n} + (c/12)m(m²−1)δ_{m+n,0}
Cardy formula: S = 2π·√(c·L₀/6)
Free boson TT OPE: T(z)T(w) ~ c/(2(z−w)⁴) + …
[L₂,L₋₂] = 4·L₀ + c/2 (exact; at c=1: 4L₀ + 1/2)
Cardy S = 2π·√(c·L₀/6); c=1, L₀=24 → 4π (exact)
Free boson: leading TT-OPE coefficient c/2 = 1/2 at c=1
Conformal-map (Joukowski transform) framework: J(z) = z + 1/z; angle-preserving
Modular invariance Z(tau+1) = Z(tau); period-1 e^{2 pi i} = 1
Partition function characters chi_p; Schur partition counting p(n)
Theorem: J(1) - 2 = 0 (Joukowski transform real-axis boundary)
Theorem: e^{2 pi i (tau+1)} - e^{2 pi i tau} = 0 (modular T-invariance)
Theorem: p(4) - 5 = 0 (number of partitions of 4 equals 5)
Virasoro algebra (2D CFT)
Primary fields + conformal weights
Modular invariance (CFT partition function)
Operator product expansion (OPE)
Conformal bootstrap (modern revival)
AdS/CFT (Maldacena 1997)
BPZ (Belavin-Polyakov-Zamolodchikov 1984)
AdS/CFT (Maldacena 1997)
c-theorem (Zamolodchikov 1986)
Bootstrap (Rattazzi 2008)
Kac determinant (1980)
WZW model (Witten 1984)
Explore the conformal-field-theory subtree on the interactive graph →