Gauge invariant input to neural network for path optimization method
arXiv:2109.11710 · doi:10.1103/PhysRevD.105.034502
Abstract
We investigate the efficiency of a gauge invariant input to a neural network for the path optimization method. While the path optimization with a completely gauge-fixed link-variable input has successfully tamed the sign problem in a simple gauge theory, the optimization does not work well when the gauge degrees of freedom remain. We propose to employ a gauge invariant input, such as plaquette, to overcome this problem. The efficiency of the gauge invariant input to the neural network is evaluated for the 2-dimensional gauge theory with a complex coupling. The average phase factor is significantly enhanced by the path optimization with the plaquette input, indicating good control of the sign problem. It opens a possibility that the path optimization is available to complicated gauge theories, including Quantum Chromodynamics, in a realistic setup.
arXiv comment7 pages, 8 figures; published version
References in corpus (35)
- Tensor renormalization group approach to 2D classical lattice models
- High density QCD on a Lefschetz thimble?
- Simulating full QCD at nonzero density using the complex Langevin equation
- Hybrid Monte Carlo on Lefschetz Thimbles -- A study of the residual sign problem
- Toward solving the sign problem with path optimization method
- Finite-Density Monte Carlo Calculations on Sign-Optimized Manifolds
- Simulating QCD at nonzero baryon density to all orders in the hopping parameter expansion
- Complex Langevin dynamics for dynamical QCD at nonzero chemical potential: a comparison with multi-parameter reweighting
- Lattice gauge equivariant convolutional neural networks
- Metropolis Monte Carlo on the Lefschetz thimble: application to a one-plaquette model
- Phase transition of four-dimensional Ising model with higher-order tensor renormalization group
- Fermions at Finite Density in (2+1)d with Sign-Optimized Manifolds
- Application of neural network to sign problem via path optimization method
- Calculating the EoS of the dense quark-gluon plasma using the Complex Langevin equation
- Applying Complex Langevin Simulations to Lattice QCD at Finite Density
- Tensor renormalization group approach to four-dimensional complex theory at finite density
- Control the model sign problem via path optimization method: Monte-Carlo approach to QCD effective model with Polyakov loop
- Path integral contour deformations for observables in gauge theory
- An improvement in complex Langevin dynamics from a view point of Lefschetz thimbles
- Worldvolume approach to the tempered Lefschetz thimble method
- Restoration of chiral symmetry in cold and dense Nambu--Jona-Lasinio model with tensor renormalization group
- Complex Langevin calculations in finite density QCD at large with the deformation technique
- A simple approach towards the sign problem using path optimisation
- Deconfinement transition line with the Complex Langevin equation up to
- Path optimization in 0+1 dimensional QCD at finite density
- Application of the path optimization method to the sign problem in an effective model of QCD with a repulsive vector-type interaction
- Complex Langevin calculations in QCD at finite density
- The topological susceptibility of two-dimensional gauge theories
- Phase transition of four-dimensional lattice theory with tensor renormalization group
- Modifying partition functions: a way to solve the sign problem
- Path optimization for gauge theory with complexified parameters
- Simulating Yang-Mills theories with a complex coupling
- Perturbative Removal of a Sign Problem
- Complex Paths Around The Sign Problem
- Statistical analysis method for the worldvolume hybrid Monte Carlo algorithm
Cited by in corpus (5)
- Exploring QCD matter in extreme conditions with Machine Learning
- Fourier-Flow model generating Feynman paths
- Improving efficiency of the path optimization method for a gauge theory
- Application of the path optimization method to a discrete spin system
- Path optimization method for the sign problem caused by fermion determinant