Abstract

We propose a general framework for finding the ground state of many-body fermionic systems by using feed-forward neural networks. The anticommutation relation for fermions is usually implemented to a variational wave function by the Slater determinant (or Pfaffian), which is a computational bottleneck because of the numerical cost of $O(N^3)$ for $N$ particles. We bypass this bottleneck by explicitly calculating the sign changes associated with particle exchanges in real space and using fully connected neural networks for optimizing the rest parts of the wave function. This reduces the computational cost to $O(N^2)$ or less. We show that the accuracy of the approximation can be improved by optimizing the "variance" of the energy simultaneously with the energy itself. We also find that a reweighting method in Monte Carlo sampling can stabilize the calculation. These improvements can be applied to other approaches based on variational Monte Carlo methods. Moreover, we show that the accuracy can be further improved by using the symmetry of the system, the representative states, and an additional neural network implementing a generalized Gutzwiller-Jastrow factor. We demonstrate the efficiency of the method by applying it to a two-dimensional Hubbard model.

Highlights

  • Recent developments in machine learning have a profound impact on the field of physics [1]

  • Various methods have been proposed in solid state physics far, such as the restricted Boltzmann machine [4,5,6,7], the convolutional neural network (CNN) [6,8,9,10,11,12], the graph convolutional network (GCN) [8], the Gaussian process state [13], and the fully connected neural network (FCNN) [14]

  • While such studies using neural networks (NNs) are successful for bosonic systems [18,19], they have encountered some difficulties for fermionic systems and frustrated spin systems due to the complicated sign structures in the wave functions [20,21]

Read more

Summary

INTRODUCTION

Recent developments in machine learning have a profound impact on the field of physics [1]. Similar methods have been applied to molecules in quantum chemistry calculations [15,16,17] While such studies using NNs are successful for bosonic systems [18,19], they have encountered some difficulties for fermionic systems and frustrated spin systems due to the complicated sign structures in the wave functions [20,21]. Numerical cost for the calculation of the Slater determinant is O(N3) for N-particle systems. We propose a general framework to approximate fermionic many-body wave functions by NNs without using the Slater determinant.

Overall framework
Markov chain Monte Carlo sampling and reweighting
Symmetry operation and representative state
Neural network architecture
Update θ
Computational cost
RESULTS
Computational details
Efficiency of the reweighting method
Two types of the neural networks
Effect of the energy variance
Irreducible representation
Parameters and samples dependence
CONCLUDING REMARKS
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.