Non-Linear Integral Equations for the SL(2,R)/U(1) black hole sigma model
arXiv:1306.2646 · doi:10.1088/1751-8113/46/41/415401
Abstract
It was previously established that the critical staggered XXZ spin chain provides a lattice regularization of the black hole CFT. We reconsider the continuum limit of this spin chain with the exact method of non-linear integral equations (NLIEs), paying particular attention to the effects of a singular integration kernel. With the help of the NLIEs, we rederive the continuous black hole spectrum, but also numerically match the density of states of the spin chain with that of the CFT, which is a new result. Finally, we briefly discuss the integrable structure of the black hole CFT and the identification of its massive integrable perturbation on the lattice.
36 pages, 12 figures
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- On the scaling behaviour of the alternating spin chain
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- Finite size spectrum of the staggered six-vertex model with -invariant boundary conditions
- Integrable boundary conditions for staggered vertex models
- An Ising-type formulation of the six-vertex model
- Finite-size effects in the spectrum of the superspin chain
- Equilibrium density matrices for the 2D black hole sigma models from an integrable spin chain
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- Non compact continuum limit of two coupled Potts models
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- On the critical behaviour of the integrable -deformed superspin chain
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- Exact surface energy of the spin chain with generic non-diagonal boundary reflections
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- Finite-size spectrum of the staggered six-vertex model with antidiagonal boundary conditions
- Scaling limit of the ground state Bethe roots for the inhomogeneous XXZ spin- chain
- The spin chain and its finite-size spectrum
- Managing Singular Kernels and Logarithmic Corrections in the Staggered Six-Vertex Model
- Factorization identities and algebraic Bethe ansatz for models
- quantum chains with quantum group invariant boundaries
- Quantum-group-invariant models: Bethe ansatz and finite-size spectrum