mlsanityData to 7 Oct 2026

Discovering Quantum Phase Transitions with Fermionic Neural Networks

arXiv 2202.05183 ↗First posted 10 Feb 2022physics.comp-ph cond-mat.other cond-mat.str-elcited by 25

Not on the map. Why?

Abstract (arXiv)

Deep neural networks have been extremely successful as highly accurate wave function ans"atze for variational Monte Carlo calculations of molecular ground states. We present an extension of one such ansatz, FermiNet, to calculations of the ground states of periodic Hamiltonians, and study the homogeneous electron gas. FermiNet calculations of the ground-state energies of small electron gas systems are in excellent agreement with previous initiator full configuration interaction quantum Monte Carlo and diffusion Monte Carlo calculations. We investigate the spin-polarized homogeneous electron gas and demonstrate that the same neural network architecture is capable of accurately representing both the delocalized Fermi liquid state and the localized Wigner crystal state. The network is given no a priori knowledge that a phase transition exists, but converges on the translationally invariant ground state at high density and spontaneously breaks the symmetry to produce the crystalline ground state at low density.

Key facts. Cited by 25 papers in the map (data through 7 Oct 2026). Builds on 1 of its 31 references that are in the map. First posted on arXiv 10 Feb 2022.

Builds on

1 of 31 references.

References · 1

  1. 2019Deep neural network solution of the electronic Schr"odinger equationcited by 124

Built on by

Cited by year (2026 to 7 Oct)

Citing papers per year: 2022: 5; 2023: 7; 2024: 4; 2025: 6; 2026: 3.

25 papers.

Sort:

  1. 2022A Self-Attention Ansatz for Ab-initio Quantum Chemistrycited by 45
  2. 2022Ab-initio quantum chemistry with neural-network wavefunctionscited by 28
  3. 2023Generalizing Neural Wave Functionscited by 26
  4. 2022Gold-standard solutions to the Schr"odinger equation using deep learning: How much physics do we need?cited by 25
  5. 2024A Kaczmarz-inspired approach to accelerate the optimization of neural network wavefunctionscited by 24
  6. 2022Sampling-free Inference for Ab-Initio Potential Energy Surface Networkscited by 19
  7. 2025An ab initio foundation model of wavefunctions that accurately describes chemical bond breakingcited by 11
  8. 2023Pairing-based graph neural network for simulating quantum materialscited by 9
  9. 2023Variational Monte Carlo on a Budget -- Fine-tuning pre-trained Neural Wavefunctionscited by 8
  10. 2024Transferable Neural Wavefunctions for Solidscited by 7
  11. 2022Deep Variational Free Energy Approach to Dense Hydrogencited by 6
  12. 2023Towards a Foundation Model for Neural Network Wavefunctionscited by 6
13 more
  1. 2023Forward Laplacian: A New Computational Framework for Neural Network-based Variational Monte Carlocited by 6
  2. 2023Convergence of variational Monte Carlo simulation and scale-invariant pre-trainingcited by 2
  3. 2025Is attention all you need to solve the correlated electron problem?cited by 2
  4. 2025The neural networks with tensor weights and emergent fermionic Wick rules in the large-width limitcited by 2
  5. 2026First-Principles AI finds crystallization of fractional quantum Hall liquidscited by 2
  6. 2026QERNEL: a Scalable Large Electron Modelcited by 2
  7. 2023Artificial intelligence for artificial materials: moir'e atomcited by 1
  8. 2025Diagonal Symmetrization of Neural Network Solvers for the Many-Electron Schr"odinger Equationcited by 1
  9. 2024Ground state phases of the two-dimension electron gas with a unified variational approachcited by 0
  10. 2024A Theoretical Framework for an Efficient Normalizing Flow-Based Solution to the Electronic Schrodinger Equationcited by 0
  11. 2025Accurate and thermodynamically consistent hydrogen equation of state for planetary modeling with flow matchingcited by 0
  12. 2025Revisiting the Broken Symmetry Phase of Solid Hydrogen: A Neural Network Variational Monte Carlo Studycited by 0
  13. 2026Predicting magnetism with first-principles AIcited by 0