Boundary entropy of integrable perturbed WZNW
arXiv:1906.01909
Abstract
We apply the recently developped analytical methods for computing the boundary entropy, or the g-function, in integrable theories with non-diagonal scattering. We consider the particular case of the current-perturbed WZNW model with boundary and compute the boundary entropy for a specific boundary condition. The main problem we encounter is that in case of non-diagonal scattering the boundary entropy is infinite. We show that this infinity can be cured by a subtraction. The difference of the boundary entropies in the UV and in the IR limits is finite, and matches the known g-functions for the unperturbed WZNW model for even values of the level.
arXiv comment27 pages, 3 figures
References in corpus (14)
- Boundary energy and boundary states in integrable quantum field theories
- Affine Toda field theory on a half line
- g-function flow in perturbed boundary conformal field theories
- The conformal boundary states for SU(2) at level 1
- Integrable quantum field theory with boundaries: the exact g-function
- Integrable theories that are asymptotically CFT
- Reflection factors and exact g-functions for purely elastic scattering theories
- Boundary TBA, trees and loops
- O(1) contribution of saddle point fluctuations to the free energy of Bethe Ansatz systems
- From A_m Trigonometric S-Matrices to the Thermodynamic Bethe Ansatz
- Exact g-function flow between conformal field theories
- Nonstandard Bethe Ansatz equations for open O(N) spin chains
- Exact g-function flows from the staircase model
- From S-matrices to the Thermodynamic Bethe Ansatz