Large- sigma model on a Euclidean torus: uniqueness and stability of the vacuum
arXiv:1905.10555 · doi:10.1007/JHEP12(2019)044
Abstract
In this paper we examine analytically the large- gap equation and its solution for the sigma model defined on a Euclidean spacetime torus of arbitrary shape and size (, being the inverse temperature. We find that the system has a unique homogeneous phase, with the fields acquiring a dynamically generated mass (analogous to the mass gap of Yang-Mills theory in ), for any and . Several related topics in the recent literature are discussed. One concerns the possibility, which turns out to be excluded according to our analysis, of a "Higgs-like" - or deconfinement - phase at small and at zero temperature. Another topics involves "soliton-like (inhomogeneous) solutions of the generalized gap equation, which we do not find. A related question concerns a possible instability of the standard vacuum on , which is shown not to occur. In all cases, the difference in the conclusions can be traced to the existence of certain zeromodes and their proper treatment. The model with twisted boundary conditions is also analyzed. The dependence and different limits involving , and are briefly discussed.
40 pages, 4 figures
References in corpus (7)
- Self-consistent crystalline condensate in chiral Gross-Neveu and Bogoliubov-de Gennes systems
- Non-Abelian vortex dynamics: Effective world-sheet action
- Topological properties of models in the large- limit
- Large-N CP(N-1) sigma model on a finite interval and the renormalized string energy
- Self-Consistent Large- Analytical Solutions of Inhomogneous Condensates in Quantum Model
- Theta-vacuum and large N limit in CP^{N-1} sigma models
- Worm Algorithm for CP(N-1) Model
Cited by in corpus (6)
- Lattice model with twisted boundary condition: bions, adiabatic continuity and pseudo-entropy
- Towards Lefschetz thimbles in Sigma models, I
- The Casimir effect for nonlinear sigma models and the Mermin-Wagner-Hohenberg-Coleman theorem
- Remarks on the large- model
- One-loop effective action of the model at large
- Lessons from models in one dimension