Construction of modular branching functions from Bethe's equations in the 3-state Potts chain

From MaRDI portal
Publication:1279260

DOI10.1007/BF01049953zbMath0945.82507arXivhep-th/9210129MaRDI QIDQ1279260

Rinat Kedem, Barry M. McCoy

Publication date: 31 May 1999

Published in: Journal of Statistical Physics (Search for Journal in Brave)

Full work available at URL: https://arxiv.org/abs/hep-th/9210129




Related Items (16)

The many faces of a characterPolynomial fermionic forms for the branching functions of the rational coset conformal field theories \(\widehat{su}(2)_M\times\widehat{su}(2)_N/\widehat{su}(2)_{M+N}\)Analytic calculation of conformal partition functions: Tricritical hard squares with fixed boundariesMultinomials and polynomial bosonic forms for the branching functions of the \(\widehat{su}(2)_{M}\times \widehat{su}(2)_{N}/\widehat{su}(2)_{M+N}\) conformal coset modelsFermionic expressions for the characters of \(c_{p,1}\) logarithmic conformal field theoriesCombinatorial constructions of modules for infinite-dimensional Lie algebras. I: Principal subspaceIntegrable anyon chains: from fusion rules to face models to effective field theories3-manifolds and VOA charactersNahm sums, quiver a-polynomials and topological recursionSpaces of coinvariants and fusion product. I: From equivalence theorem to Kostka polynomialsFermionic characters and arbitrary highest-weight integrable \({\widehat{\mathfrak{sl}}}_{r+1}\)-modulesZnclock models and chains ofso(n)2non-Abelian anyons: symmetries, integrable points and low energy propertiesVirtual crystals and fermionic formulas of type 𝐷_{𝑛+1}⁽²⁾, 𝐴_{2𝑛}⁽²⁾, and 𝐶_{𝑛}⁽¹⁾Fermionic counting of RSOS states and Virasoro character formulas for the unitary minimal series \(M(\nu,\nu+1)\): Exact resultsAnyonic interpretation of Virasoro characters and the thermodynamic Bethe ansatzNumerical results for the three-state critical Potts model on finite rectangular lattices.



Cites Work


This page was built for publication: Construction of modular branching functions from Bethe's equations in the 3-state Potts chain