Two-Flavor Lattice QCD with a Finite Density of Heavy Quarks: Heavy-Dense Limit and "Particle-Hole" Symmetry
arXiv:1509.00087 · doi:10.1007/JHEP02(2016)051
Abstract
We investigate the properties of the half-filling point in lattice QCD (LQCD), in particular the disappearance of the sign problem and the emergence of an apparent particle-hole symmetry, and try to understand where these properties come from by studying the heavy-dense fermion determinant and the corresponding strong-coupling partition function (which can be integrated analytically). We then add in a first step an effective Polyakov loop gauge action (which reproduces the leading terms in the character expansion of the Wilson gauge action) to the heavy-dense partition function and try to analyze how some of the properties of the half-filling point change when leaving the strong coupling limit. In a second step, we take also the leading nearest-neighbor fermion hopping terms into account (including gauge interactions in the fundamental representation) and mention how the method could be improved further to incorporate the full set of nearest-neighbor fermion hoppings. Using our mean-field method, we also obtain an approximate (,T) phase diagram for heavy-dense LQCD at finite inverse gauge coupling . Finally, we propose a simple criterion to identify the chemical potential beyond which lattice artifacts become dominant.
39 pages, 22 figures
References in corpus (3)
Cited by in corpus (8)
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- Applying Complex Langevin Simulations to Lattice QCD at Finite Density
- Anatomy of the sign-problem in heavy-dense QCD
- Equation of state for cold and dense heavy QCD
- Towards a theoretical description of dense QCD
- Nonanalyticity, sign problem and Polyakov line in Z3-symmetric heavy quark model at low temperature: Phenomenological model analyses