Fermionic Quasi-Particle Representations for Characters of (G(1))1 × (G(1))1 (G(1))2

Abstract

We present fermionic quasi-particle sum representations for some of the characters (or branching functions) of ~(G(1))1 × (G(1))1 (G(1))2 ~for all simply-laced Lie algebras G. For given G the characters are written as the partition function of a set of rank~G types of massless quasi-particles in certain charge sectors, with nontrivial lower bounds on the one-particle momenta. We discuss the non-uniqueness of the representations for the identity character of the critical Ising model, which arises in both the A1 and E8 cases.

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