Finite Density States in Integrable Conformal Field Theories
arXiv:hep-th/0408162 · doi:10.1142/9789812775344_0031
Abstract
We study states of large charge density in integrable conformal coset models. For the O(2) coset, we consider two different S-matrices, one corresponding to a Thirring mass perturbation and the other to the continuation to O(2+epsilon). The former leads to simplification in the conformal limit; the latter gives a more complicated description of the O(2) system, with a large zero mode sector in addition to the right- and left-movers. We argue that for the conformal O(2+2M|2M) supergroup coset, the S-matrix is given by the analog of the O(2+epsilon) construction.
21 pages. To appear in "From Fields to Strings: Circumnavigating Theoretical Physics," in memory of Ian Kogan. v. 2: added references
Cited by in corpus (14)
- Giant Magnons
- Planar N=4 Gauge Theory and the Hubbard Model
- The AdS5xS5 Superstring in Light-Cone Gauge and its Bethe Equations
- Connecting giant magnons to the pp-wave: An interpolating limit of
- Bethe Ansatz for a Quantum Supercoset Sigma Model
- Dressing the Giant Magnon II
- Strings as Multi-Particle States of Quantum Sigma-Models
- Asymptotic Bethe Ansatz from String Sigma Model on S^3 x R
- Boundary Spectra in Superspace Sigma-Models
- Spin Models and Superconformal Yang-Mills Theory
- Nesting and Dressing
- Sugawara form for AdS superstring
- Edge states and conformal boundary conditions in super spin chains and super sigma models
- The SU(2) Long Range Bethe Ansatz and Continuous Integrable Systems