The Nambu-Jona-Lasinio model reduced to 2+1 dimensions has two different path integral formulations: at finite chemical potential one formulation has a severe sign problem similar to that found in QCD, while the other does not. At large N, where N is the number of flavors, one can compute the probability distributions of fermion correlators analytically in both formulations. In the former case one finds a broad distribution with small mean; in the latter one finds a heavy tailed positive distribution amenable to the cumulant expansion techniques developed in earlier work. We speculate on the implications of this model for QCD. © 2013 American Physical Society
Thesis (Ph.D.)--University of Washington, 2017-08The theory of quantum chromodynamics (QCD) encodes ...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
Finite volume QCD close to the chiral limit cannot be described by chiral Perturbation Theory using ...
Due to the presence of light pions in the theory, lattice QCD at finite densities suffers from issue...
Abstract. Due to the presence of light pions in the theory, lattice QCD at finite densities suffers ...
We show how sign problems in simulations of many-body systems can manifest themselves in the form of...
We show how sign problems in simulations of many-body systems can manifest themselves in the form of...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We study the distribution of the phase angle and the magnitude of the fermion determinant as well as...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We identify the global symmetries of SU(2) lattice gauge theory with N flavors of staggered fermion...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
Thesis (Ph.D.)--University of Washington, 2017-08The theory of quantum chromodynamics (QCD) encodes ...
Thesis (Ph.D.)--University of Washington, 2017-08The theory of quantum chromodynamics (QCD) encodes ...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
Finite volume QCD close to the chiral limit cannot be described by chiral Perturbation Theory using ...
Due to the presence of light pions in the theory, lattice QCD at finite densities suffers from issue...
Abstract. Due to the presence of light pions in the theory, lattice QCD at finite densities suffers ...
We show how sign problems in simulations of many-body systems can manifest themselves in the form of...
We show how sign problems in simulations of many-body systems can manifest themselves in the form of...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We study the distribution of the phase angle and the magnitude of the fermion determinant as well as...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
We identify the global symmetries of SU(2) lattice gauge theory with N flavors of staggered fermion...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
Thesis (Ph.D.)--University of Washington, 2017-08The theory of quantum chromodynamics (QCD) encodes ...
Thesis (Ph.D.)--University of Washington, 2017-08The theory of quantum chromodynamics (QCD) encodes ...
We generalize QCD at asymptotically large isospin chemical potential to an arbitrary even number of ...
Finite volume QCD close to the chiral limit cannot be described by chiral Perturbation Theory using ...