Abstract: We apply complex Langevin dynamics to chiral random matrix theory at nonzero chemical potential. At large quark mass the simulations agree with the analytical results while incorrect convergence is found for small quark masses. The region of quark masses for which the complex Langevin dynamics converges incorrectly is identified as the region where the fermion determinant frequently traces out a path surrounding the origin of the complex plane during the Langevin flow. This links the incorrect convergence to an ambiguity in the Langevin force due to the presence of the logarithm of the fermion determinant in the action. ar X i
The three-dimensional SU(3) spin model is an effective Polyakov loop model for QCD at nonzero temper...
Lattice QCD at non-vanishing chemical potential is studied using the complex Langevin equation (CLE)...
AbstractComplex Langevin dynamics can solve the sign problem appearing in numerical simulations of t...
We study a random matrix model for QCD at finite density via complex Langevin dynamics. This model h...
Abstract Recently the complex Langevin method (CLM) has been attracting attention as a solution to t...
In this paper we test the complex Langevin algorithm for numerical simulations of a random matrix mo...
We study the Stephanov model, which is an RMT model for QCD at finite density, using the Complex Lan...
Abstract QCD at nonzero baryon chemical potential suffers from the sign problem, due to the complex ...
The sign problem appears in lattice QCD as soon as a non-zero chemical potential is introduced. This...
The sign problem at nonzero chemical potential prohibits the use of importance sampling in lattice s...
In this thesis we give self-sufficient introduction to the complex Langevin method, which is a promi...
I review the presence of the sign problem in lattice QCD at nonzero baryon density and its relation ...
We simulate lattice QCD at finite quark-number chemical potential to study nuclear matter, using the...
AbstractWe show that complex Langevin simulation converges to a wrong result within the semiclassica...
The three-dimensional SU(3) spin model is an effective Polyakov loop model for QCD at nonzero temper...
Lattice QCD at non-vanishing chemical potential is studied using the complex Langevin equation (CLE)...
AbstractComplex Langevin dynamics can solve the sign problem appearing in numerical simulations of t...
We study a random matrix model for QCD at finite density via complex Langevin dynamics. This model h...
Abstract Recently the complex Langevin method (CLM) has been attracting attention as a solution to t...
In this paper we test the complex Langevin algorithm for numerical simulations of a random matrix mo...
We study the Stephanov model, which is an RMT model for QCD at finite density, using the Complex Lan...
Abstract QCD at nonzero baryon chemical potential suffers from the sign problem, due to the complex ...
The sign problem appears in lattice QCD as soon as a non-zero chemical potential is introduced. This...
The sign problem at nonzero chemical potential prohibits the use of importance sampling in lattice s...
In this thesis we give self-sufficient introduction to the complex Langevin method, which is a promi...
I review the presence of the sign problem in lattice QCD at nonzero baryon density and its relation ...
We simulate lattice QCD at finite quark-number chemical potential to study nuclear matter, using the...
AbstractWe show that complex Langevin simulation converges to a wrong result within the semiclassica...
The three-dimensional SU(3) spin model is an effective Polyakov loop model for QCD at nonzero temper...
Lattice QCD at non-vanishing chemical potential is studied using the complex Langevin equation (CLE)...
AbstractComplex Langevin dynamics can solve the sign problem appearing in numerical simulations of t...