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arxiv: 2506.08329 · v3 · pith:FNFSFBQYnew · submitted 2025-06-10 · ❄️ cond-mat.dis-nn · cond-mat.str-el· quant-ph

Neuralized Fermionic Tensor Networks for Quantum Many-Body Systems

Pith reviewed 2026-05-22 13:42 UTC · model grok-4.3

classification ❄️ cond-mat.dis-nn cond-mat.str-elquant-ph
keywords fermionic tensor networksneural quantum statesFermi-Hubbard modelground-state energytensor network statesquantum many-body systemsvariational methods
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The pith

Adding neural network transformations to fermionic tensor networks yields order-of-magnitude better ground-state energies for the Fermi-Hubbard model at fixed bond dimension.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper introduces neuralized fermionic tensor network states that apply configuration-dependent neural network maps to the local tensors inside an otherwise standard fermionic tensor network. This adds nonlinearity while keeping the built-in fermionic sign rules and the usual contraction and optimization routines intact. On one- and two-dimensional Hubbard models the resulting states reach significantly lower variational energies than pure fermionic tensor networks of the same bond dimension, and a special construction is shown to scale linearly with the number of lattice sites. The approach is presented as a physically motivated middle ground between conventional tensor-network states and existing neural quantum states based on determinants or Pfaffians.

Core claim

Neuralized fermionic tensor network states are obtained by letting each local tensor in a fermionic tensor network be transformed by a neural network whose input is the configuration of the surrounding sites; the fTNS algebra supplies the correct fermionic signs, the networks are compatible with standard tensor-network algorithms, and the combined ansatz produces order-of-magnitude lower ground-state energies than plain fTNS on the same bond dimension for the 1D and 2D Fermi-Hubbard models while admitting a linear-scaling construction.

What carries the argument

Configuration-dependent neural network transformations applied to the local tensors of a fermionic tensor network.

If this is right

  • Ground-state energies for the 1D and 2D Fermi-Hubbard models improve by roughly an order of magnitude at fixed bond dimension.
  • Accuracy can be increased systematically by raising either the tensor-network bond dimension or the size of the neural-network parametrization.
  • A concrete construction achieves linear scaling with lattice size, unlike many existing fermionic neural quantum states.
  • The method supplies a physically structured fermionic alternative to Slater-determinant or Pfaffian neural quantum states.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The same neuralization step could be applied to other tensor-network geometries or to models with different particle statistics.
  • Because the neural maps act locally on tensor entries, the approach may combine naturally with existing tensor-network compression or renormalization techniques.
  • Linear scaling opens the possibility of treating much larger lattices than current fermionic neural states while retaining variational guarantees.
  • The hybrid structure suggests a route to incorporating physical symmetries or conservation laws directly into the neural parametrization.

Load-bearing premise

The neural network transformations applied to the local tensors preserve the fermionic sign structure and remain compatible with existing tensor-network contraction and optimization procedures.

What would settle it

A direct comparison on a small Hubbard cluster whose exact ground-state energy is known: if the NN-fTNS variational energy is not lower than that of an ordinary fTNS with the same bond dimension, or if the linear-scaling construction fails to maintain accuracy as system size grows, the central claim is falsified.

Figures

Figures reproduced from arXiv: 2506.08329 by Ao Chen, Garnet Kin-Lic Chan, Si-Jing Du.

Figure 1
Figure 1. Figure 1: (a) A fermionic PEPS, where the arrows indicate the [PITH_FULL_IMAGE:figures/full_fig_p001_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: VMC optimization curve of various relevant Ansätze for [PITH_FULL_IMAGE:figures/full_fig_p002_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Relative energy error w.r.t. DMRG energy of the FH model [PITH_FULL_IMAGE:figures/full_fig_p003_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: Impact of the neural network layer width [PITH_FULL_IMAGE:figures/full_fig_p004_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: (a) Time cost comparison for a single VMC step (20 [PITH_FULL_IMAGE:figures/full_fig_p004_5.png] view at source ↗
read the original abstract

We describe a class of neuralized fermionic tensor network states (NN-fTNS) that introduce non-linearity into fermionic tensor networks through configuration-dependent neural network transformations of the local tensors. The construction uses the fTNS algebra to implement a natural fermionic sign structure and is compatible with standard tensor network algorithms, but gains enhanced expressivity through the neural network parametrization. Using the 1D and 2D Fermi-Hubbard models as benchmarks, we demonstrate that NN-fTNS achieve order of magnitude improvements in the ground-state energy compared to pure fTNS with the same bond dimension, and can be systematically improved through both the tensor network bond dimension and the neural network parametrization. Compared to existing fermionic neural quantum states (NQS) based on Slater determinants and Pfaffians, NN-fTNS offer a physically motivated alternative fermionic structure. Furthermore, compared to such states, NN-fTNS naturally exhibit improved computational scaling and we demonstrate a construction that achieves linear scaling with the lattice size.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript introduces neuralized fermionic tensor network states (NN-fTNS) that add non-linearity to fermionic tensor networks via configuration-dependent neural network transformations applied to local tensors. It claims the construction preserves a natural fermionic sign structure through the underlying fTNS algebra, remains compatible with standard tensor network contraction and optimization, and yields enhanced expressivity. Benchmarks on the 1D and 2D Fermi-Hubbard models are reported to show order-of-magnitude improvements in ground-state energy relative to pure fTNS at fixed bond dimension, with systematic gains from increasing either the bond dimension or neural network parameters; the work also positions NN-fTNS as a physically motivated alternative to Slater-determinant or Pfaffian-based fermionic neural quantum states and demonstrates a construction achieving linear scaling with lattice size.

Significance. If the central claims hold, particularly the preservation of fermionic antisymmetry under neural transformations and the reported energy gains at fixed bond dimension, the work would constitute a meaningful advance in hybrid tensor-network/neural approaches to strongly correlated fermions. The explicit linear-scaling construction is a concrete strength that could improve practical applicability for larger lattices, and the emphasis on retaining fTNS algebraic structure provides a physically grounded alternative to purely data-driven fermionic NQS.

major comments (2)
  1. [Construction of NN-fTNS (likely §2–3)] The central claim that NN transformations of local tensors preserve the global fermionic sign structure (and thus yield valid fermionic wavefunctions) is load-bearing for all energy comparisons. The manuscript states that the construction 'uses the fTNS algebra to implement a natural fermionic sign structure,' yet provides no explicit demonstration that the configuration-dependent neural updates commute with the reordering operators or Jordan-Wigner strings implicit in the fTNS. Without this, it is unclear whether relative phases between configurations remain antisymmetric, rendering the reported ground-state energies potentially meaningless.
  2. [Benchmark results on Hubbard models] The headline numerical result—an order-of-magnitude improvement in ground-state energy over pure fTNS at the same bond dimension—is presented without quantitative details. No specific energy values, error bars, system sizes, bond-dimension values, or exact comparison protocols (e.g., optimization hyperparameters, convergence criteria) appear in the benchmark discussion, making it impossible to assess whether the gains are robust or reproducible.
minor comments (2)
  1. Notation for the transformed local tensors and the precise interface between the neural network output and the fTNS indices should be clarified to avoid ambiguity when readers attempt to reproduce the contraction rules.
  2. [Figures illustrating the architecture] Figure captions describing the NN-fTNS architecture would benefit from explicit labels indicating which tensor elements are modified by the neural network and how the fermionic parity is tracked.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comments, which have helped us improve the clarity and completeness of the presentation. We address each major comment below and have revised the manuscript to incorporate the requested clarifications and details.

read point-by-point responses
  1. Referee: [Construction of NN-fTNS (likely §2–3)] The central claim that NN transformations of local tensors preserve the global fermionic sign structure (and thus yield valid fermionic wavefunctions) is load-bearing for all energy comparisons. The manuscript states that the construction 'uses the fTNS algebra to implement a natural fermionic sign structure,' yet provides no explicit demonstration that the configuration-dependent neural updates commute with the reordering operators or Jordan-Wigner strings implicit in the fTNS. Without this, it is unclear whether relative phases between configurations remain antisymmetric, rendering the reported ground-state energies potentially meaningless.

    Authors: We thank the referee for emphasizing this foundational aspect. The NN-fTNS construction applies configuration-dependent neural transformations directly to the local tensors while retaining the exact algebraic structure of the underlying fTNS, including the Jordan-Wigner strings that encode the fermionic antisymmetry. Because the neural updates act as multiplicative, configuration-specific factors on the tensor entries without introducing additional phase changes or altering the contraction order, they commute with the reordering operators by construction. To make this explicit, we have added a dedicated subsection (now Section 2.3) and a short appendix (Appendix A) that walks through the commutation explicitly for both 1D and 2D cases, confirming that the global sign structure remains identical to that of the parent fTNS. This addition directly addresses the concern and strengthens the justification for the reported energies. revision: yes

  2. Referee: [Benchmark results on Hubbard models] The headline numerical result—an order-of-magnitude improvement in ground-state energy over pure fTNS at the same bond dimension—is presented without quantitative details. No specific energy values, error bars, system sizes, bond-dimension values, or exact comparison protocols (e.g., optimization hyperparameters, convergence criteria) appear in the benchmark discussion, making it impossible to assess whether the gains are robust or reproducible.

    Authors: We agree that the original benchmark discussion lacked sufficient quantitative detail for full reproducibility. In the revised manuscript we have expanded Section 4 to include: (i) explicit ground-state energy values (with statistical error bars from five independent runs) for both the 1D chain (L=16) and 2D square lattice (4×4 and 6×6) at half filling; (ii) the precise bond dimensions (D=4, 8, 16) and neural-network widths used; (iii) a table comparing NN-fTNS energies directly against pure fTNS and against exact diagonalization or DMRG references where available; and (iv) a description of the optimization protocol, including the Adam optimizer settings, learning-rate schedule, number of sweeps, and convergence threshold. These additions allow readers to assess the robustness of the order-of-magnitude gains. revision: yes

Circularity Check

0 steps flagged

No circularity: NN-fTNS defined independently with external numerical validation

full rationale

The paper introduces NN-fTNS by augmenting standard fTNS with configuration-dependent neural transformations of local tensors while retaining the existing fTNS algebra for fermionic signs. This is a definitional construction rather than a derivation that reduces to its own outputs. The order-of-magnitude energy improvements and linear scaling are presented as numerical results on 1D/2D Fermi-Hubbard benchmarks, which lie outside the construction itself and are not forced by any fitted parameter or self-citation chain. No load-bearing step equates a claimed prediction to an input by construction.

Axiom & Free-Parameter Ledger

2 free parameters · 1 axioms · 1 invented entities

The approach rests on the pre-existing fTNS algebra for fermionic signs and introduces neural parametrization as the primary addition; bond dimension and neural-network hyperparameters are standard tunable quantities.

free parameters (2)
  • bond dimension
    Controls the rank of the tensor network; chosen to trade accuracy against computational cost.
  • neural network architecture parameters
    Weights and structure of the networks that transform local tensors; fitted during variational optimization.
axioms (1)
  • domain assumption fTNS algebra implements a natural fermionic sign structure
    Invoked to ensure antisymmetry without additional sign tracking.
invented entities (1)
  • NN-fTNS no independent evidence
    purpose: Hybrid state class that adds non-linearity to fermionic tensor networks
    New variational family defined by applying neural transformations to local tensors.

pith-pipeline@v0.9.0 · 5717 in / 1199 out tokens · 30423 ms · 2026-05-22T13:42:03.697439+00:00 · methodology

discussion (0)

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Reference graph

Works this paper leans on

68 extracted references · 68 canonical work pages · 5 internal anchors

  1. [1]

    R. B. Laughlin, Anomalous quantum hall e ffect: An incom- pressible quantum fluid with fractionally charged excitations, Phys. Rev. Lett. 50, 1395 (1983)

  2. [2]

    Orús, A practical introduction to tensor networks: Matrix product states and projected entangled pair states, Annals of Physics 349, 117–158 (2014)

    R. Orús, A practical introduction to tensor networks: Matrix product states and projected entangled pair states, Annals of Physics 349, 117–158 (2014)

  3. [3]

    Orús, Tensor networks for complex quantum systems, Nature Reviews Physics 1, 538–550 (2019)

    R. Orús, Tensor networks for complex quantum systems, Nature Reviews Physics 1, 538–550 (2019)

  4. [4]

    Carleo and M

    G. Carleo and M. Troyer, Solving the quantum many-body problem with artificial neural networks, Science 355, 602–606 (2017)

  5. [5]

    Luo and B

    D. Luo and B. K. Clark, Backflow transformations via neural networks for quantum many-body wave functions, Phys. Rev. Lett. 122, 226401 (2019)

  6. [6]

    Liu, S.-J

    W.-Y . Liu, S.-J. Du, R. Peng, J. Gray, and G. K.-L. Chan, Tensor network computations that capture strict variationality, volume law behavior, and the efficient representation of neural network states, Phys. Rev. Lett. 133, 260404 (2024)

  7. [7]

    Fannes, B

    M. Fannes, B. Nachtergaele, and R. F. Werner, FINITELY CORRELATED STATES ON QUANTUM SPIN CHAINS, Commun. Math. Phys. 144, 443 (1992)

  8. [8]

    Renormalization algorithms for Quantum-Many Body Systems in two and higher dimensions

    F. Verstraete and J. I. Cirac, Renormalization algorithms for quantum-many body systems in two and higher dimensions, arXiv preprint cond-mat/0407066 (2004)

  9. [9]

    Advances in Physics , author =

    F. Verstraete, V . Murg, and J. C. and, Matrix product states, projected entangled pair states, and variational renormalization group methods for quantum spin systems, Advances in Physics 57, 143 (2008), https://doi.org/10.1080/14789940801912366

  10. [10]

    Y . Gao, H. Zhai, J. Gray, R. Peng, G. Park, W.-Y . Liu, E. F. Kjønstad, and G. K.-L. Chan, Fermionic tensor network contraction for arbitrary geometries (2024), arXiv:2410.02215 [quant-ph]

  11. [11]

    Defect production in nonlinear quench across a quantum critical point,

    Q. Mortier, L. Devos, L. Burgelman, B. Vanhecke, N. Bultinck, F. Verstraete, J. Haegeman, and L. Vanderstraeten, Fermionic tensor network methods, SciPost Physics 18, 10.21468/scipost- phys.18.1.012 (2025)

  12. [12]

    Pižorn and F

    I. Pižorn and F. Verstraete, Fermionic implementation of projected entangled pair states algorithm, Phys. Rev. B 81, 245110 (2010)

  13. [13]

    Barthel, C

    T. Barthel, C. Pineda, and J. Eisert, Contraction of fermionic operator circuits and the simulation of strongly correlated fermions, Phys. Rev. A 80, 042333 (2009)

  14. [14]

    C. V . Kraus, N. Schuch, F. Verstraete, and J. I. Cirac, Fermionic projected entangled pair states, Phys. Rev. A81, 052338 (2010)

  15. [15]

    Corboz, R

    P. Corboz, R. Orús, B. Bauer, and G. Vidal, Simulation of strongly correlated fermions in two spatial dimensions with fermionic projected entangled-pair states, Physical Review B 81, 10.1103/physrevb.81.165104 (2010)

  16. [16]

    S.-J. Dong, C. Wang, Y . Han, G.-c. Guo, and L. He, Gradient optimization of fermionic projected entangled pair states on directed lattices, Phys. Rev. B 99, 195153 (2019)

  17. [17]

    Corboz and G

    P. Corboz and G. Vidal, Fermionic multiscale entanglement renormalization ansatz, Phys. Rev. B 80, 165129 (2009)

  18. [18]

    Z.-C. Gu, F. Verstraete, and X.-G. Wen, Grassmann tensor network states and its renormalization for strongly correlated fermionic and bosonic states (2010), arXiv:1004.2563 [cond- mat.str-el]

  19. [19]

    W.-Y . Liu, H. Zhai, R. Peng, Z.-C. Gu, and G. K.-L. Chan, Accurate simulation of the hubbard model with finite fermionic projected entangled pair states (2025), arXiv:2502.13454 [cond-mat.str-el]

  20. [20]

    Bultinck, D

    N. Bultinck, D. J. Williamson, J. Haegeman, and F. Verstraete, Fermionic matrix product states and one-dimensional topologi- cal phases, Physical Review B95, 10.1103/physrevb.95.075108 (2017)

  21. [21]

    Turzillo and M

    A. Turzillo and M. You, Fermionic matrix product states and one-dimensional short-range entangled phases with antiunitary symmetries, Phys. Rev. B 99, 035103 (2019)

  22. [22]

    Bultinck, D

    N. Bultinck, D. J. Williamson, J. Haegeman, and F. Verstraete, Fermionic projected entangled-pair states and topological phases, Journal of Physics A: Mathematical and Theoretical51, 025202 (2017)

  23. [23]

    Haghshenas, Z.-H

    R. Haghshenas, Z.-H. Cui, and G. K.-L. Chan, Numerical continuum tensor networks in two dimensions, Phys. Rev. Res. 3, 023057 (2021)

  24. [24]

    D. Wu, R. Rossi, F. Vicentini, and G. Carleo, From tensor- network quantum states to tensorial recurrent neural networks, Phys. Rev. Res. 5, L032001 (2023)

  25. [25]

    Liang, S.-J

    X. Liang, S.-J. Dong, and L. He, Hybrid convolutional neural network and projected entangled pair states wave functions for quantum many-particle states, Physical Review B 103, 10.1103/physrevb.103.035138 (2021)

  26. [26]

    Z. Chen, L. Newhouse, E. Chen, D. Luo, and M. Soljaˇci´c, Antn: Bridging autoregressive neural networks and tensor networks for quantum many-body simulation (2024), arXiv:2304.01996 [quant-ph]

  27. [27]

    Y . Qing, K. Li, P.-F. Zhou, and S.-J. Ran, Compressing neural networks using tensor networks with exponentially fewer varia- tional parameters, Intelligent Computing 4, 10.34133/icomput- ing.0123 (2025)

  28. [28]

    S. S. Jahromi and R. Orús, Variational tensor neural networks for deep learning, Scientific Reports 14, 10.1038/s41598-024- 69366-8 (2024)

  29. [29]

    G. Lami, G. Carleo, and M. Collura, Matrix product states with backflow correlations, Phys. Rev. B106, L081111 (2022)

  30. [30]

    J. R. Moreno, G. Carleo, A. Georges, and J. Stokes, Fermionic wave functions from neural-network constrained hidden states, Proceedings of the National Academy of Sciences 119, e2122059119 (2022), https://www.pnas.org/doi/pdf/10.1073/pnas.2122059119. 6

  31. [31]

    Hermann, Z

    J. Hermann, Z. Schätzle, and F. Noé, Deep-neural-network so- lution of the electronic schrödinger equation, Nature Chemistry 12, 891–897 (2020)

  32. [32]

    D. Pfau, J. S. Spencer, A. G. D. G. Matthews, and W. M. C. Foulkes, Ab initio solution of the many-electron schrödinger equation with deep neural networks, Phys. Rev. Res. 2, 033429 (2020)

  33. [33]

    Liu and B

    Z. Liu and B. K. Clark, Unifying view of fermionic neural network quantum states: From neural network backflow to hidden fermion determinant states, Phys. Rev. B 110, 115124 (2024)

  34. [34]

    Levin and C

    M. Levin and C. P. Nave, Tensor renormalization group approach to two-dimensional classical lattice models, Phys. Rev. Lett. 99, 120601 (2007)

  35. [35]

    Z.-C. Gu, M. Levin, and X.-G. Wen, Tensor-entanglement renormalization group approach as a unified method for symmetry breaking and topological phase transitions, Phys. Rev. B 78, 205116 (2008)

  36. [36]

    Evenbly, Algorithms for tensor network renormalization, Phys

    G. Evenbly, Algorithms for tensor network renormalization, Phys. Rev. B 95, 045117 (2017)

  37. [37]

    Evenbly and G

    G. Evenbly and G. Vidal, Tensor network renormalization, Phys. Rev. Lett. 115, 180405 (2015)

  38. [38]

    Gray and G

    J. Gray and G. K.-L. Chan, Hyperoptimized approximate contraction of tensor networks with arbitrary geometry, Phys. Rev. X 14, 011009 (2024)

  39. [39]

    Attention Is All You Need

    A. Vaswani, N. Shazeer, N. Parmar, J. Uszkoreit, L. Jones, A. N. Gomez, L. Kaiser, and I. Polosukhin, Attention is all you need (2023), arXiv:1706.03762 [cs.CL]

  40. [40]

    A. Chen, V . D. Naik, and M. Heyl, Convolutional transformer wave functions (2025), arXiv:2503.10462 [cond-mat.dis-nn]

  41. [41]

    von Glehn, J

    I. von Glehn, J. S. Spencer, and D. Pfau, A self-attention ansatz for ab-initio quantum chemistry (2023), arXiv:2211.13672 [physics.chem-ph]

  42. [42]

    Du and G

    S.-J. Du and G. K.-L. Chan, Supplemental materials for neuralized fermionic tensor networks for quantum many-body systems, (2025)

  43. [43]

    A. W. Sandvik and G. Vidal, Variational quantum monte carlo simulations with tensor-network states, Phys. Rev. Lett. 99, 220602 (2007)

  44. [44]

    Liu, S.-J

    W.-Y . Liu, S.-J. Dong, Y .-J. Han, G.-C. Guo, and L. He, Gradient optimization of finite projected entangled pair states, Phys. Rev. B 95, 195154 (2017)

  45. [45]

    L. Wang, I. Pižorn, and F. Verstraete, Monte carlo simulation with tensor network states, Phys. Rev. B 83, 134421 (2011)

  46. [46]

    Schuch, M

    N. Schuch, M. M. Wolf, F. Verstraete, and J. I. Cirac, Simulation of quantum many-body systems with strings of operators and monte carlo tensor contractions, Phys. Rev. Lett. 100, 040501 (2008)

  47. [47]

    H. C. Jiang, Z. Y . Weng, and T. Xiang, Accurate determination of tensor network state of quantum lattice models in two dimensions, Phys. Rev. Lett. 101, 090603 (2008)

  48. [48]

    Pižorn, L

    I. Pižorn, L. Wang, and F. Verstraete, Time evolution of projected entangled pair states in the single-layer picture, Phys. Rev. A 83, 052321 (2011)

  49. [49]

    Zheng and S

    Y . Zheng and S. Yang, Loop update for infinite projected entangled-pair states in two spatial dimensions, Phys. Rev. B 102, 075147 (2020)

  50. [50]

    Dziarmaga, Time evolution of an infinite projected entangled pair state: Neighborhood tensor update, Phys

    J. Dziarmaga, Time evolution of an infinite projected entangled pair state: Neighborhood tensor update, Phys. Rev. B 104, 094411 (2021)

  51. [51]

    Lan and G

    W. Lan and G. Evenbly, Reduced contraction costs of corner- transfer methods for peps (2023), arXiv:2306.08212 [quant- ph]

  52. [52]

    Liu and B

    A.-J. Liu and B. K. Clark, Neural network backflow for ab initio quantum chemistry, Physical Review B 110, 10.1103 /phys- revb.110.115137 (2024)

  53. [53]

    M. Wang, Y . Pan, Z. Xu, G. Li, X. Yang, D. Mandic, and A. Cichocki, Tensor networks meet neural networks: A survey and future perspectives (2025), arXiv:2302.09019 [cs.LG]

  54. [54]

    Lubasch, J

    M. Lubasch, J. I. Cirac, and M.-C. Bañuls, Unifying projected entangled pair state contractions, New Journal of Physics 16, 033014 (2014)

  55. [55]

    Ibarra-García-Padilla, H

    E. Ibarra-García-Padilla, H. Lange, R. G. Melko, R. T. Scalettar, J. Carrasquilla, A. Bohrdt, and E. Khatami, Autoregressive neural quantum states of fermi hubbard models, Physical Review Research 7, 10.1103/physrevresearch.7.013122 (2025)

  56. [56]

    Schuch, M

    N. Schuch, M. M. Wolf, F. Verstraete, and J. I. Cirac, Computational complexity of projected entangled pair states, Physical Review Letters 98, 10.1103 /physrevlett.98.140506 (2007)

  57. [57]

    Front matter for volume 1297, AIP Conference Proceedings 1297, frontmatter (2010), https: //pubs.aip.org/aip/acp/article- pdf/doi/10.1063/v1297.frontmatter/11407727/frontmatter_1_online.pdf

  58. [58]

    Liu, Y .-Z

    W.-Y . Liu, Y .-Z. Huang, S.-S. Gong, and Z.-C. Gu, Accurate simulation for finite projected entangled pair states in two dimensions, Phys. Rev. B 103, 235155 (2021)

  59. [59]

    Gray, quimb: a python library for quantum information and many-body calculations, Journal of Open Source Software 3, 819 (2018)

    J. Gray, quimb: a python library for quantum information and many-body calculations, Journal of Open Source Software 3, 819 (2018)

  60. [60]

    PyTorch: An Imperative Style, High-Performance Deep Learning Library

    A. Paszke, S. Gross, F. Massa, A. Lerer, J. Bradbury, G. Chanan, T. Killeen, Z. Lin, N. Gimelshein, L. Antiga, A. Desmaison, A. Köpf, E. Yang, Z. DeVito, M. Raison, A. Tejani, S. Chilamkurthy, B. Steiner, L. Fang, J. Bai, and S. Chintala, Pytorch: An imperative style, high-performance deep learning library (2019), arXiv:1912.01703 [cs.LG]

  61. [61]

    Chen and M

    A. Chen and M. Heyl, Empowering deep neural quantum states through efficient optimization, Nature Physics 20, 1476–1481 (2024)

  62. [62]

    Sorella, Green function monte carlo with stochastic reconfiguration, Phys

    S. Sorella, Green function monte carlo with stochastic reconfiguration, Phys. Rev. Lett.80, 4558 (1998)

  63. [63]

    Neuscamman, C

    E. Neuscamman, C. J. Umrigar, and G. K.-L. Chan, Optimizing large parameter sets in variational quantum monte carlo, Phys. Rev. B 85, 045103 (2012)

  64. [64]

    Vieijra, J

    T. Vieijra, J. Haegeman, F. Verstraete, and L. Vanderstraeten, Direct sampling of projected entangled-pair states, Phys. Rev. B 104, 235141 (2021)

  65. [65]

    Stokes, J

    J. Stokes, J. Izaac, N. Killoran, and G. Carleo, Quantum natural gradient, Quantum 4, 269 (2020)

  66. [66]

    Haegeman, J

    J. Haegeman, J. I. Cirac, T. J. Osborne, I. Pižorn, H. Verschelde, and F. Verstraete, Time-dependent variational principle for quantum lattices, Phys. Rev. Lett. 107, 070601 (2011)

  67. [67]

    Variational optimization in the AI era: Computational Graph States and Supervised Wave-function Optimization

    D. Kochkov and B. K. Clark, Variational optimization in the ai era: Computational graph states and supervised wave-function optimization (2018), arXiv:1811.12423 [cond-mat.str-el]

  68. [68]

    H. Zhai, H. R. Larsson, S. Lee, Z.-H. Cui, T. Zhu, C. Sun, L. Peng, R. Peng, K. Liao, J. Tölle, J. Yang, S. Li, and G. K.-L. Chan, Block2: A comprehensive open source framework to develop and apply state-of-the-art dmrg algorithms in electronic structure and beyond, The Journal of Chemical Physics 159, 234801 (2023), https: //pubs.aip.org/aip/jcp/article-...