quantum-many-body-leaderboard

mcp
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SUMMARY

QMBL: the Quantum Many-Body Leaderboard. The best published ground-state energies for lattice models, hydrogen chains and the electron gas, with a JSON API and an MCP server for agents.

README.md
QMBL: the Quantum Many-Body Leaderboard

DOI
License: Apache 2.0
agents: API · MCP

A live record of SOTA published ground-state energies for lattice models, hydrogen chains and the electron gas.

Organised literature for fellow researchers and AI systems. So that we can see the works of the wider research community at one glance, build on each other's work more efficiently and advance frontier science together.

AI agents and crawlers: read qmbl.org/llms.txt for what the data means and where it is, and the JSON API under qmbl.org/api/.

Use QMBL with your agent

  • Paste this prompt into your favorite agent:

    Use QMBL: the Quantum Many-Body Leaderboard (qmbl.org) to answer my questions about ground-state energies. First read https://qmbl.org/llms.txt. Then use the JSON API it describes: https://qmbl.org/api/models.json lists the models, https://qmbl.org/api/m/<model>.json gives every instance of one model with its exact and best energies, and https://qmbl.org/api/i/<instance_id>.json gives every published energy of one instance.
    
  • Or add the MCP server. Paste this prompt into your favorite agent:

    Add the QMBL MCP server: download https://raw.githubusercontent.com/quantum-many-body-leaderboard/quantum-many-body-leaderboard/main/mcp/server.mjs and register it as a local stdio MCP server named "qmbl" that runs `node <path to server.mjs>`.
    

Leaderboard

All 1121 Hamiltonian instances, 31 of them infinite lattices (click a model to expand)

Heisenberg: 121 instances, energies as E/N (S.S)
instance value energy method code
chain, 20 sites, open exact -0.4341237 ED Wu et al. (2024) run script
best variational -0.4341237 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 20 sites exact -0.4452193 ED Wu et al. (2024) run script
best variational -0.4452193 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 200 sites, open exact -0.4422078 Exact solution McCulloch (code) Uni20-dev/bethe, QMBL check
best variational -0.4422078 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 200 sites exact -0.4431678 Exact solution McCulloch (code) Uni20-dev/bethe, QMBL check
best variational -0.4431678 (+<1e-7) DMRG Wu et al. (2024) run script
checkerboard, infinite lattice best variational -0.513442(1) variational wave function Schäfer et al. (2023)
best extrapolated -0.5132(2) DMRG Schäfer et al. (2023)
best approximate -0.5138(2) NLCE Schäfer et al. (2023)
checkerboard, infinite lattice, S = 1 best variational -1.5339(5) variational wave function Schäfer et al. (2023)
best extrapolated -1.532(1) DMRG Schäfer et al. (2023)
best approximate -1.533(2) NLCE Schäfer et al. (2023)
crossedruby, infinite lattice best variational -0.48946(5) variational wave function Schäfer et al. (2023)
best extrapolated -0.4865(7) DMRG Schäfer et al. (2023)
best approximate -0.492(1) NLCE Schäfer et al. (2023)
crossedruby, infinite lattice, S = 1 best variational -1.490(1) variational wave function Schäfer et al. (2023)
best extrapolated -1.4764(5) DMRG Schäfer et al. (2023)
best approximate -1.489(5) NLCE Schäfer et al. (2023)
honeycomb 7x7 (98 sites) best variational -0.5421(4) VMC (LCN) Fu et al. (2022)
kagome, infinite lattice best extrapolated -0.4386(5) DMRG Depenbrock et al. (2012)
kagome-24, 24 sites exact -0.4412486 ED Läuchli et al. (2011)
kagome 2x2 (12 sites) exact -0.4537396 ED Läuchli et al. (2011)
kagome 2x3 (18 sites) exact -0.4471262 ED Wu et al. (2024) run script
best variational -0.4471262 (+<1e-7) DMRG Wu et al. (2024) run script
kagome-30, 30 sites exact -0.4384773 ED Läuchli et al. (2011)
kagome-36a, 36 sites exact -0.4385521 ED Läuchli et al. (2011)
kagome-36b, 36 sites exact -0.4390813 ED Läuchli et al. (2011)
kagome-36c, 36 sites exact -0.4392871 ED Läuchli et al. (2011)
kagome-36d, 36 sites exact -0.4383765 ED Läuchli et al. (2011)
kagome-42a, 42 sites exact -0.437999 ED Läuchli et al. (2011)
kagome-42b, 42 sites exact -0.4381426 ED Läuchli et al. (2011)
kagome 4x4 (48 sites) exact -0.4387039 ED Wietek & Läuchli (2018)
best variational -0.4375(2) (+1.2e-3) VMC (GCNN) Đurić et al. (2024) uses NetKet
best extrapolated -0.4383(2) (+4.0e-4) DMRG Depenbrock et al. (2012)
kagome 6x6 (108 sites) best extrapolated -0.4383(3) DMRG Depenbrock et al. (2012)
kagome 8x8 (192 sites) best variational -0.42987(1) VMC (Gutzwiller) Wu et al. (2024) run script
pyrochlore, infinite lattice best variational -0.489472(8) variational wave function Schäfer et al. (2023)
best extrapolated -0.490(6) DMRG Hagymási et al. (2020)
best approximate -0.49(1) NLCE Hagymási et al. (2020)
pyrochlore, infinite lattice, S = 1 best variational -1.490(1) variational wave function Schäfer et al. (2023)
best approximate -1.489(5) NLCE Schäfer et al. (2023)
pyrochlore 2x2x2 (32 sites) exact -0.5168588 ED QMBL check, checks/pyrochlore-32-ed/ QMBL code
best variational -0.5162(1) (+6.6e-4) VMC (PP) Astrakhantsev et al. (2021) uses mVMC
best extrapolated -0.5168 ○ (+5.9e-5) DMRG Hagymási et al. (2020)
pyrochlore 2x2x2 (128 sites) best variational -0.49229(7) VMC (PP + RBM) Pohle et al. (2023) uses mVMC
best extrapolated -0.49434(5) VMC (PP) Pohle et al. (2023) uses mVMC
pyrochlore 2x2x3 (48 sites) best variational -0.5028(2) VMC (PP) Astrakhantsev et al. (2021) uses mVMC
pyrochlore 2x2x4 (64 sites) best variational -0.4924(2) VMC (PP) Astrakhantsev et al. (2021) uses mVMC
pyrochlore 2x2x6 (96 sites) best variational -0.4917(4) VMC (PP) Astrakhantsev et al. (2021) uses mVMC
pyrochlore 2x4x6 (192 sites) best variational -0.4915(2) VMC (PP) Astrakhantsev et al. (2021) uses mVMC
pyrochlore 3x3x3 (108 sites) best variational -0.4871(1) VMC (PP) Astrakhantsev et al. (2021) uses mVMC
pyrochlore 3x3x3 (432 sites) best variational -0.48851(3) VMC (PP) Pohle et al. (2023) uses mVMC
best extrapolated -0.4924(2) VMC (PP) Pohle et al. (2023) uses mVMC
pyrochlore 4x4x4 (256 sites) best variational -0.485584(3) VMC (RVB) Cheng & Li (2026)
pyrochlore 4x4x4 (1024 sites) best variational -0.48800(1) VMC (PP) Pohle et al. (2023) run script
best extrapolated -0.4921(2) VMC (PP) Pohle et al. (2023) uses mVMC
rectangular 10x20, periodic/open exact (stochastic) -0.6599522(4) SSE QMC Sandvik (2026)
rectangular 12x24, periodic/open exact (stochastic) -0.6612549(4) SSE QMC Sandvik (2026)
rectangular 14x28, periodic/open exact (stochastic) -0.6622809(4) SSE QMC Sandvik (2026)
rectangular 16x32, periodic/open exact (stochastic) -0.6630939(4) SSE QMC Sandvik (2026)
rectangular 18x36, periodic/open exact (stochastic) -0.6637496(4) SSE QMC Sandvik (2026)
rectangular 20x40, periodic/open exact (stochastic) -0.6642865(4) SSE QMC Sandvik (2026)
rectangular 24x48, periodic/open exact (stochastic) -0.6651098(6) SSE QMC Sandvik (2026)
rectangular 32x64, periodic/open exact (stochastic) -0.6661668(6) SSE QMC Sandvik (2026)
rectangular 48x96, periodic/open exact (stochastic) -0.6672462(6) SSE QMC Sandvik (2026)
rectangular 4x8, periodic/open exact (stochastic) -0.6623181(4) SSE QMC Sandvik (2026)
rectangular 64x128, periodic/open exact (stochastic) -0.6677918(4) SSE QMC Sandvik (2026)
rectangular 6x12, periodic/open exact (stochastic) -0.6570101(4) SSE QMC Sandvik (2026)
rectangular 6x8 exact -0.6759867 ED Wietek & Läuchli (2018)
rectangular 8x16, periodic/open exact (stochastic) -0.6583592(4) SSE QMC Sandvik (2026)
shuriken, 24 sites exact -0.4483291 ED Astrakhantsev et al. (2021)
shuriken, 96 sites best variational -0.43826(1) VMC (PP) Wu et al. (2024) uses mVMC
shuriken, 216 sites best variational -0.4376(1) VMC (PP) Wu et al. (2024) uses mVMC
shuriken, 384 sites best variational -0.4371(1) VMC (PP) Wu et al. (2024) uses mVMC
square 4x4 exact -0.7017802 ED Wu et al. (2024) run script
best variational -0.7017449 (+3.5e-5) VQE Wu et al. (2024) run script
square 6x6, open exact -0.6035218 ED Wu et al. (2024) run script
best variational -0.6035218 ○ (+<1e-7) DMRG Huang et al. (2016)
best extrapolated -0.60351496(1) (+6.9e-6) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 6x6 exact -0.6788721 ED Richter et al. (2004)
best variational -0.678871(3) (+1.1e-6) VMC (CNN BF + RBM) Hendry et al. (2025) uses NetKet
best extrapolated -0.67887177(7) (+3.8e-7) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square, 38 sites exact -0.6779156 ED Richter et al. (2004)
square, 40 sites exact -0.6773713 ED Richter et al. (2004)
square, 50 sites exact -0.675102 ED Wietek & Läuchli (2018)
square 8x8, open exact (stochastic) -0.6190371(2) SSE QMC Sandvik (2026)
best variational -0.619034(6) (+2.7e-6) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 8x8 exact (stochastic) -0.67349005(2) SSE QMC Sandvik (2026)
best variational -0.6735 ○ (−1.0e-5) VMC (HQT) Guo et al. (2026) uses NetKet
square 10x10, open exact (stochastic) -0.6286561(2) SSE QMC Sandvik (2026)
best variational -0.628656(9) (+1.2e-7) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
best extrapolated -0.628657(5) (−8.8e-7) DMRG Wu et al. (2024) run script
square 10x10 exact (stochastic) -0.67155266(2) SSE QMC Sandvik (2026)
best variational -0.67155260(3) (+6.0e-8) VMC (ResNet) Chen & Heyl (2023) ChenAo-Phys/MinSR
square 12x12, open exact (stochastic) -0.6352007(2) SSE QMC Sandvik (2026)
best variational -0.635201(7) (+1.3e-7) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 12x12 exact (stochastic) -0.67068192(2) SSE QMC Sandvik (2026)
best variational -0.67062(2) (+6.3e-5) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 14x14, open exact (stochastic) -0.6399410(2) SSE QMC Sandvik (2026)
best variational -0.639929(6) (+1.2e-5) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 14x14 exact (stochastic) -0.67023225(2) SSE QMC Sandvik (2026)
best variational -0.67014(2) (+9.4e-5) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 16x16, open exact (stochastic) -0.6435317(2) SSE QMC Sandvik (2026)
best variational -0.643522(7) (+9.8e-6) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 16x16 exact (stochastic) -0.66997660(2) SSE QMC Sandvik (2026)
best variational -0.66987(2) (+1.1e-4) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
best extrapolated -0.6699687(9) (+7.9e-6) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 18x18, open exact (stochastic) -0.6463451(4) SSE QMC Sandvik (2026)
best variational -0.646337(5) (+8.6e-6) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 18x18 exact (stochastic) -0.66982043(2) SSE QMC Sandvik (2026)
best variational -0.66968(2) (+1.4e-4) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
best extrapolated -0.6697819(5) (+3.9e-5) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 20x20, open exact (stochastic) -0.6486091(4) SSE QMC Sandvik (2026)
best variational -0.648590(5) (+1.9e-5) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 20x20 exact (stochastic) -0.66971967(2) SSE QMC Sandvik (2026)
best variational -0.66959(1) (+1.3e-4) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 22x22, open exact (stochastic) -0.6504689(4) SSE QMC Sandvik (2026)
best variational -0.650253(5) (+2.2e-4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 22x22 exact (stochastic) -0.66965176(2) SSE QMC Sandvik (2026)
square 24x24, open exact (stochastic) -0.6520251(4) SSE QMC Sandvik (2026)
best variational -0.651982(7) (+4.3e-5) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 24x24 exact (stochastic) -0.66960434(2) SSE QMC Sandvik (2026)
best variational -0.66944(2) (+1.7e-4) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 26x26, open exact (stochastic) -0.6533456(4) SSE QMC Sandvik (2026)
best variational -0.653129(5) (+2.2e-4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 26x26 exact (stochastic) -0.66957017(3) SSE QMC Sandvik (2026)
square 28x28, open exact (stochastic) -0.6544806(4) SSE QMC Sandvik (2026)
best variational -0.654261(4) (+2.2e-4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 28x28 exact (stochastic) -0.66954496(3) SSE QMC Sandvik (2026)
best variational -0.66937(1) (+1.7e-4) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 30x30, open best variational -0.655241(4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 30x30 exact (stochastic) -0.66952595(3) SSE QMC Sandvik (2026)
square 32x32, open exact (stochastic) -0.6563289(4) SSE QMC Sandvik (2026)
best variational -0.656089(4) (+2.4e-4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 32x32 exact (stochastic) -0.66951133(3) SSE QMC Sandvik (2026)
best variational -0.66930(1) (+2.2e-4) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
best extrapolated -0.6694877(4) (+2.4e-5) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
square 36x36, open best variational -0.657523(4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 36x36 exact (stochastic) -0.66949091(3) SSE QMC Sandvik (2026)
square 40x40, open best variational -0.658657(4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 40x40 exact (stochastic) -0.66947776(3) SSE QMC Sandvik (2026)
square 44x44, open best variational -0.659565(4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 44x44 exact (stochastic) -0.66946889(3) SSE QMC Sandvik (2026)
square 46x46, open best variational -0.659941(4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 48x48, open exact (stochastic) -0.6606690(4) SSE QMC Sandvik (2026)
best variational -0.660323(4) (+3.5e-4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 48x48 exact (stochastic) -0.66946274(3) SSE QMC Sandvik (2026)
square 50x50, open best variational -0.660649(3) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 52x52, open best variational -0.660967(4) VMC (minGRU) Merali et al. (2026) ParallelScan-RNNs/PSR-NQS
square 52x52 exact (stochastic) -0.66945833(3) SSE QMC Sandvik (2026)
square 56x56 exact (stochastic) -0.66945502(3) SSE QMC Sandvik (2026)
square 60x60 exact (stochastic) -0.66945260(3) SSE QMC Sandvik (2026)
square 64x64, open exact (stochastic) -0.6628515(4) SSE QMC Sandvik (2026)
square 64x64 exact (stochastic) -0.66945072(3) SSE QMC Sandvik (2026)
square 72x72 exact (stochastic) -0.66944815(3) SSE QMC Sandvik (2026)
square 80x80 exact (stochastic) -0.66944645(3) SSE QMC Sandvik (2026)
square 88x88 exact (stochastic) -0.66944530(3) SSE QMC Sandvik (2026)
square 96x96, open exact (stochastic) -0.6650415(2) SSE QMC Sandvik (2026)
square 96x96 exact (stochastic) -0.66944454(3) SSE QMC Sandvik (2026)
square 128x128, open exact (stochastic) -0.6661389(2) SSE QMC Sandvik (2026)
square, infinite lattice best variational -0.6693781 ○ iPEPS Rader & Läuchli (2018)
best extrapolated -0.669441878(9) SSE QMC Sandvik (2026)
triangular 4x4 exact -0.5347197 ED Wu et al. (2024) run script
best variational -0.5347197 (−<1e-7) DMRG Wu et al. (2024) run script
triangular 6x6 exact -0.5603734 ED Wu et al. (2024) run script
best variational -0.560313(3) (+6.0e-5) VMC (GCNN) Roth et al. (2022) uses NetKet
triangular, 48 sites exact -0.558603 ED Wietek & Läuchli (2018)
triangular 10x10, open best variational -0.5147668 DMRG Wu et al. (2024) run script
triangular, 108 sites best variational -0.55315(3) VMC (GCNN) Roth et al. (2022) uses NetKet
triangular 12x12, open best variational -0.5150648 DMRG Wu et al. (2024) run script
triangular 12x12 best variational -0.5493(1) VMC (2D RNN) Moss et al. (2025) mschuylermoss/HeisenbergRNN
triangular 14x14, open best variational -0.5138(1) VMC (2D RNN) Wu et al. (2024) run script
triangular 16x16, open best variational -0.51668(9) VMC (2D RNN) Wu et al. (2024) run script
triangular 18x18 best variational -0.551703(1) VMC (ViT) Viteritti et al. (2026)
best extrapolated -0.55200(1) VMC (ViT) Viteritti et al. (2026)
triangular 24x24 best variational -0.551602(1) VMC (ViT) Viteritti et al. (2026)
best extrapolated -0.55189(1) VMC (ViT) Viteritti et al. (2026)
triangular 30x30 best variational -0.551528(1) VMC (ViT) Viteritti et al. (2026)
best extrapolated -0.55180(1) VMC (ViT) Viteritti et al. (2026)
triangular 42x42 best variational -0.551429(1) VMC (ViT) Viteritti et al. (2026)
best extrapolated -0.55171(1) VMC (ViT) Viteritti et al. (2026)
J1-J2: 113 instances, energies as E/N (S.S)
instance value energy method code
honeycomb 7x7 (98 sites), J2 = 0.2 best variational -0.4538(4) VMC (LCN) Fu et al. (2022)
rectangular 4x6, J2 = 0.5 exact -0.5225249 ED Wu et al. (2024) run script
best variational -0.5225249 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, J2 = 0.05 exact -0.68059 ED Wu et al. (2024) run script
best variational -0.6805657 (+2.4e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.1 exact -0.6598172 ED Wu et al. (2024) run script
best variational -0.6597832 (+3.4e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.15 exact -0.6395429 ED Wu et al. (2024) run script
best variational -0.6395107 (+3.2e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.2 exact -0.6198739 ED Wu et al. (2024) run script
best variational -0.6198639 (+1.0e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.25 exact -0.6009545 ED Wu et al. (2024) run script
best variational -0.6009332 (+2.1e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.3 exact -0.5829838 ED Wu et al. (2024) run script
best variational -0.5829522 (+3.2e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.35 exact -0.5662448 ED Wu et al. (2024) run script
best variational -0.5662285 (+1.6e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.4 exact -0.5511478 ED Wu et al. (2024) run script
best variational -0.5511135 (+3.4e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.45 exact -0.5382998 ED Wu et al. (2024) run script
best variational -0.5382766 (+2.3e-5) VQE Wu et al. (2024) run script
best extrapolated -0.5370(4) (+1.3e-3) cluster update (TPS) Wang et al. (2011)
square 4x4, J2 = 0.5 exact -0.5286202 ED Wu et al. (2024) run script
best variational -0.5286202 (−<1e-7) DMRG Wu et al. (2024) run script
best extrapolated -0.5268(4) (+1.8e-3) cluster update (TPS) Wang et al. (2011)
square 4x4, J2 = 0.6 exact -0.5258958 ED Wu et al. (2024) run script
best variational -0.5258158 (+8.0e-5) VQE Wu et al. (2024) run script
best extrapolated -0.518(2) (+8.2e-3) cluster update (TPS) Wang et al. (2011)
square 4x4, J2 = 0.65 exact -0.5393825 ED Wu et al. (2024) run script
best variational -0.5393444 (+3.8e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.7 exact -0.5638581 ED Wu et al. (2024) run script
best variational -0.5637716 (+8.7e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.75 exact -0.5942731 ED Wu et al. (2024) run script
best variational -0.5942152 (+5.8e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.8 exact -0.6273351 ED Wu et al. (2024) run script
best variational -0.6273137 (+2.1e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.85 exact -0.6617197 ED Wu et al. (2024) run script
best variational -0.6617069 (+1.3e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.9 exact -0.6968656 ED Wu et al. (2024) run script
best variational -0.6967967 (+6.9e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 0.95 exact -0.7324989 ED Wu et al. (2024) run script
best variational -0.7324804 (+1.8e-5) VQE Wu et al. (2024) run script
square 4x4, J2 = 1 exact -0.7684681 ED Wu et al. (2024) run script
best variational -0.7684501 (+1.8e-5) VQE Wu et al. (2024) run script
square 6x6, J2 = 0.1 exact -0.638096 ED Schulz et al. (1996)
best variational -0.638078 ○ (+1.8e-5) VMC (ViT) Golubev et al. (2026) uses NetKet
square 6x6, J2 = 0.2 exact -0.5990463 ED Schulz et al. (1996)
best variational -0.599044 ○ (+2.3e-6) VMC (ViT) Golubev et al. (2026) uses NetKet
square 6x6, J2 = 0.3 exact -0.5624595 ED Wu et al. (2024) run script
best variational -0.562453 ○ (+6.5e-6) VMC (ViT) Golubev et al. (2026) uses NetKet
square 6x6, J2 = 0.4 exact -0.529745 ED Wu et al. (2024) run script
best variational -0.529744 ○ (+1.0e-6) DMRG Gong et al. (2013)
best extrapolated -0.529747(1) (−2.0e-6) DMRG Gong et al. (2013)
square 6x6, J2 = 0.45 exact -0.5156574 ED QMBL check, checks/exact-recompute-2026-09/ QMBL code
best variational -0.515655 ○ (+2.4e-6) DMRG Gong et al. (2013)
best extrapolated -0.51566(1) (−2.6e-6) VMC (Gutzwiller) Hu et al. (2013)
square 6x6, J2 = 0.5 exact -0.5038097 ED Wu et al. (2024) run script
best variational -0.503805 ○ (+4.7e-6) DMRG Gong et al. (2013)
best projected -0.5033(4) (+5.1e-4) FN-GFMC (PEPS) Lin et al. (2024)
best extrapolated -0.50382(1) (−1.0e-5) VMC (Gutzwiller) Hu et al. (2013)
square 6x6, J2 = 0.55 exact -0.4951777 ED Schulz et al. (1996)
best variational -0.495167 ○ (+1.1e-5) DMRG Gong et al. (2013)
best projected -0.4939(5) (+1.3e-3) FN-GFMC (PEPS) Lin et al. (2024)
best extrapolated -0.49521(7) (−3.2e-5) VMC (Gutzwiller) Hu et al. (2013)
square 6x6, J2 = 0.6 exact -0.4932386 ED Wu et al. (2024) run script
best variational -0.49318(5) (+5.9e-5) VMC (RBM) Chen et al. (2022)
best extrapolated -0.488(1) (+5.3e-3) cluster update (TPS) Wang et al. (2011)
square 6x6, J2 = 0.65 exact -0.5065879 ED Schulz et al. (1996)
best variational -0.506299 ○ (+2.9e-4) VMC (ViT) Golubev et al. (2026) uses NetKet
square 6x6, J2 = 0.7 exact -0.5300012 ED Schulz et al. (1996) run script
best variational -0.5299243 (+7.7e-5) DMRG Wu et al. (2024) run script
square 6x6, J2 = 0.8 exact -0.5864866 ED Schulz et al. (1996) run script
best variational -0.586411(9) (+7.6e-5) VMC (RBM) Chen et al. (2022)
square 6x6, J2 = 0.9 exact -0.649052 ED Schulz et al. (1996) run script
best variational -0.6478705 (+1.2e-3) DMRG Wu et al. (2024) run script
square 6x6, J2 = 1 exact -0.7143604 ED Schulz et al. (1996) run script
best variational -0.71429(1) (+7.0e-5) VMC (RBM) Chen et al. (2022)
square, 40 sites, J2 = 0.1 exact -0.6366151 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.2 exact -0.5975117 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.3 exact -0.5606822 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.4 exact -0.5272092 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.5 exact -0.4990762 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.55 exact -0.4879479 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.6 exact -0.4796232 ED QMBL check, checks/j1j2-40-sector-ed/ QMBL code
square, 40 sites, J2 = 0.65 exact -0.5011508 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.7 exact -0.5263826 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.8 exact -0.5835051 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 0.9 exact -0.6459228 ED Richter & Schulenburg (2009)
square, 40 sites, J2 = 1 exact -0.7109702 ED Richter & Schulenburg (2009)
square 8x8, J2 = 0.1 best variational -0.633093 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 8x8, J2 = 0.2 best variational -0.594508 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 8x8, J2 = 0.3 best variational -0.558295 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 8x8, J2 = 0.4 best variational -0.525653(1) VMC (RBM + PP) Nomura & Imada (2021) uses mVMC
best extrapolated -0.5262(1) DMRG Gong et al. (2013)
square 8x8, J2 = 0.45 best variational -0.511331(1) VMC (RBM + PP) Nomura & Imada (2021) uses mVMC
best extrapolated -0.5116(1) DMRG Gong et al. (2013)
square 8x8, J2 = 0.48 best extrapolated -0.5034(4) cluster update (TPS) Wang et al. (2011)
square 8x8, J2 = 0.5 best variational -0.498963(2) VMC (RBM + PP) Wu et al. (2024) uses mVMC
best extrapolated -0.4992(1) DMRG Gong et al. (2013)
square 8x8, J2 = 0.52 best extrapolated -0.4941(1) cluster update (TPS) Wang et al. (2011)
square 8x8, J2 = 0.55 best variational -0.488820(2) VMC (RBM + PP) Nomura & Imada (2021) uses mVMC
best extrapolated -0.4891(1) DMRG Gong et al. (2013)
square 8x8, J2 = 0.6 best variational -0.481606 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
best extrapolated -0.4808(9) cluster update (TPS) Wang et al. (2011)
square 8x8, J2 = 0.65 best variational -0.498312 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 8x8, J2 = 0.7 best variational -0.522091 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 8x8, J2 = 0.8 best variational -0.57731 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 8x8, J2 = 0.9 best variational -0.637518 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 8x8, J2 = 1 best variational -0.700508 ○ VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 0.1 best variational -0.631365 † VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 0.2 best variational -0.592982 † VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 0.3 best variational -0.556912 † VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 0.4 best variational -0.524361 † VMC (ViT) Golubev et al. (2026) uses NetKet
best extrapolated -0.5253 ○ DMRG Gong et al. (2013)
square 10x10, J2 = 0.44 best variational -0.51273 ○ VMC (CNN) Li et al. (2022)
square 10x10, J2 = 0.45 best variational -0.51001(1) VMC (Gutzwiller) Hu et al. (2013)
best extrapolated -0.511 ○ DMRG Gong et al. (2013)
square 10x10, J2 = 0.46 best variational -0.50744 ○ VMC (CNN) Liang et al. (2023)
square 10x10, J2 = 0.48 best variational -0.50231 ○ VMC (CNN) Liang et al. (2023)
square 10x10, J2 = 0.5 best variational -0.4976939(2) VMC (CNN-MPS) Fan et al. (2026)
best projected -0.4957(2) FN-GFMC (PEPS) Lin et al. (2024)
best extrapolated -0.4988 ○ DMRG Gong et al. (2013)
square 10x10, J2 = 0.55 best variational -0.48693(3) VMC (Gutzwiller) Hu et al. (2013)
best projected -0.4853(4) FN-GFMC (PEPS) Lin et al. (2024)
best extrapolated -0.488 ○ DMRG Gong et al. (2013)
square 10x10, J2 = 0.6 best variational -0.47839 ○ VMC (CNN) Liang et al. (2023)
square 10x10, J2 = 0.65 best variational -0.494672 † VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 0.7 best variational -0.519035 † VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 0.8 best variational -0.57413 † VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 0.9 best variational -0.63417 † VMC (ViT) Golubev et al. (2026) uses NetKet
square 10x10, J2 = 1 best variational -0.69670(2) VMC (RBM) Chen et al. (2022)
square 12x12, J2 = 0.44 best variational -0.51225 ○ VMC (CNN) Li et al. (2022)
square 12x12, J2 = 0.45 best extrapolated -0.5088(1) cluster update (TPS) Wang et al. (2011)
square 12x12, J2 = 0.46 best variational -0.50697 ○ VMC (CNN) Liang et al. (2023)
square 12x12, J2 = 0.48 best variational -0.50183 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.5008(1) cluster update (TPS) Wang et al. (2011)
square 12x12, J2 = 0.5 best variational -0.496989 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.4963(2) cluster update (TPS) Wang et al. (2011)
square 12x12, J2 = 0.52 best extrapolated -0.4920(1) cluster update (TPS) Wang et al. (2011)
square 12x12, J2 = 0.55 best variational -0.48607(1) VMC (GCNN) Roth et al. (2022) uses NetKet
best extrapolated -0.4862(2) cluster update (TPS) Wang et al. (2011)
square 12x12, J2 = 0.6 best variational -0.47715 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.4784(3) cluster update (TPS) Wang et al. (2011)
square 14x14, J2 = 0.4 best variational -0.52287(1) VMC (Gutzwiller) Hu et al. (2013)
best extrapolated -0.52351(2) VMC (Gutzwiller) Hu et al. (2013)
square 14x14, J2 = 0.44 best variational -0.512 ○ VMC (CNN) Li et al. (2022)
square 14x14, J2 = 0.45 best variational -0.50899(1) VMC (Gutzwiller) Hu et al. (2013)
best extrapolated -0.50953(1) VMC (Gutzwiller) Hu et al. (2013)
square 14x14, J2 = 0.46 best variational -0.50675 ○ VMC (CNN) Liang et al. (2023)
square 14x14, J2 = 0.48 best variational -0.50159 ○ VMC (CNN) Liang et al. (2023)
square 14x14, J2 = 0.5 best variational -0.49674 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.49722(2) VMC (Gutzwiller) Hu et al. (2013)
square 14x14, J2 = 0.55 best variational -0.48581 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.48696(5) VMC (Gutzwiller) Hu et al. (2013)
square 14x14, J2 = 0.6 best variational -0.47678 ○ VMC (CNN) Liang et al. (2023)
square 16x16, J2 = 0.44 best variational -0.51188 ○ VMC (CNN) Li et al. (2022)
square 16x16, J2 = 0.45 best extrapolated -0.5087(1) cluster update (TPS) Wang et al. (2011)
square 16x16, J2 = 0.46 best variational -0.50662 ○ VMC (CNN) Liang et al. (2023)
square 16x16, J2 = 0.48 best variational -0.50147 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.5008(2) cluster update (TPS) Wang et al. (2011)
square 16x16, J2 = 0.5 best variational -0.4969140(5) VMC (CNN-MPS) Fan et al. (2026)
best extrapolated -0.4966(3) cluster update (TPS) Wang et al. (2011)
square 16x16, J2 = 0.52 best extrapolated -0.4920(1) cluster update (TPS) Wang et al. (2011)
square 16x16, J2 = 0.55 best variational -0.48565 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.4859(4) cluster update (TPS) Wang et al. (2011)
square 16x16, J2 = 0.6 best variational -0.47656 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.4777(3) cluster update (TPS) Wang et al. (2011)
square 18x18, J2 = 0.4 best variational -0.52259(1) VMC (Gutzwiller) Hu et al. (2013)
best extrapolated -0.52333(1) VMC (Gutzwiller) Hu et al. (2013)
square 18x18, J2 = 0.44 best variational -0.51179 ○ VMC (CNN) Li et al. (2022)
square 18x18, J2 = 0.45 best variational -0.50874(1) VMC (Gutzwiller) Hu et al. (2013)
best extrapolated -0.50940(1) VMC (Gutzwiller) Hu et al. (2013)
square 18x18, J2 = 0.46 best variational -0.50651 ○ VMC (CNN) Liang et al. (2023)
square 18x18, J2 = 0.48 best variational -0.50139 ○ VMC (CNN) Liang et al. (2023)
square 18x18, J2 = 0.5 best variational -0.496513 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.49717(2) VMC (Gutzwiller) Hu et al. (2013)
square 18x18, J2 = 0.55 best variational -0.48557 ○ VMC (CNN) Liang et al. (2023)
best extrapolated -0.48698(5) VMC (Gutzwiller) Hu et al. (2013)
square 18x18, J2 = 0.6 best variational -0.47652 ○ VMC (CNN) Liang et al. (2023)
square 20x20, J2 = 0.5 best variational -0.4967987(6) VMC (CNN-MPS) Fan et al. (2026)
best extrapolated -0.49684(1) VMC (ViT) Viteritti et al. (2026)
triangular, 48 sites, J2 = 0.125 exact -0.5173144 ED Wu et al. (2024)
triangular, 108 sites, J2 = 0.125 best variational -0.51268(9) VMC (GCNN) Roth et al. (2022) uses NetKet
triangular 12x12, J2 = 0.125 best variational -0.51218(9) VMC (GCNN) Roth et al. (2022) uses NetKet
Kitaev (K-J-Γ): 7 instances, energies as E/N (S.S)
instance value energy method code
honeycomb 11x11 (242 sites), open, K = -1, J = 0, Gamma = 0 exact -0.1882584 Exact solution Lin et al. (2022)
best variational -0.1820213 ○ (+6.2e-3) DMRG Lin et al. (2022)
best projected -0.1867058 ○ (+1.6e-3) DMRG² (isoTNS) Lin et al. (2022)
honeycomb 3x4 (24 sites), K = -1, J = 0, Gamma = 0 exact -0.1988727 ED Kurita et al. (2015)
best variational -0.19887(2) (−2.3e-6) VMC (PP) Kurita et al. (2015)
honeycomb 4x4 (32 sites), K = -1, J = 0, Gamma = 0 exact -0.1963139 ED Kurita et al. (2015)
best variational -0.19617(8) (+1.4e-4) VMC (PP) Kurita et al. (2015)
honeycomb 5x5 (50 sites), open, K = -1, J = 0, Gamma = 0 exact -0.178506 Exact solution Lin et al. (2022)
best variational -0.1785027 ○ (+3.3e-6) DMRG Lin et al. (2022)
best projected -0.1767248 ○ (+1.8e-3) DMRG² (isoTNS) Lin et al. (2022)
honeycomb 6x6 (72 sites), periodic/open, K = 1, J = 0, Gamma = 0 exact -0.1891314 Exact solution Jin et al. (2021)
honeycomb 7x7 (98 sites), open, K = -1, J = 0, Gamma = 0 exact -0.1835418 Exact solution Lin et al. (2022)
best variational -0.1826 ○ (+9.4e-4) DMRG Lin et al. (2022)
best projected -0.1824684 ○ (+1.1e-3) DMRG² (isoTNS) Lin et al. (2022)
honeycomb-hex24, 24 sites, K = -1, J = 0, Gamma = 0 exact -0.1985125 ED Kurita et al. (2015)
best variational -0.198510(6) (+2.1e-6) VMC (PP) Kurita et al. (2015)
Shastry-Sutherland: 29 instances, energies as E/N (S.S)
instance value energy method code
square 4x4, J = 0.7, Jd = 1 exact -0.3968907 ED Munehisa & Munehisa (2004)
square 6x6, J = 0.5, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square 6x6, J = 0.66697792, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square 6x6, J = 0.67441, Jd = 1 exact -0.375004 ED Sindermann et al. (2006)
square 6x6, J = 0.675, Jd = 1 exact -0.3752862 ED Sindermann et al. (2006)
square 6x6, J = 0.68, Jd = 1 exact -0.3777047 ED Sindermann et al. (2006)
square 6x6, J = 0.7, Jd = 1 exact -0.3885784 ED Sindermann et al. (2006)
square 6x6, J = 0.8, Jd = 1 exact -0.4517531 ED Sindermann et al. (2006)
best variational -0.451717(6) (+3.6e-5) VMC (ConvNeXt) Nutakki et al. (2025) NeuralQXLab/convnextnnqs
best extrapolated -0.45175 ○ (+3.1e-6) VMC (Transformer) Viteritti et al. (2025)
square 6x6, J = 0.85, Jd = 1 exact -0.4843341 ED Sindermann et al. (2006)
square 8x8, J = 0.8, Jd = 1 best variational -0.449829 ○ VMC (Transformer) Viteritti et al. (2025)
best extrapolated -0.44995 ○ VMC (Transformer) Viteritti et al. (2025)
square 10x10, J = 0.8, Jd = 1 best variational -0.449342(4) VMC (ConvNeXt) Nutakki et al. (2025) NeuralQXLab/convnextnnqs
best extrapolated -0.44947 ○ VMC (Transformer) Viteritti et al. (2025)
square 12x12, J = 0.7, Jd = 1 best variational -0.37627 ○ VMC (Gutzwiller) Chen & Liu (2026)
square 12x12, J = 0.8, Jd = 1 best variational -0.449078 ○ VMC (Transformer) Viteritti et al. (2025)
best extrapolated -0.44931 ○ VMC (Transformer) Viteritti et al. (2025)
square 14x14, J = 0.8, Jd = 1 best variational -0.448929 ○ VMC (Transformer) Viteritti et al. (2025)
best extrapolated -0.4492 ○ VMC (Transformer) Viteritti et al. (2025)
square 16x16, J = 0.7, Jd = 1 best variational -0.37642 ○ VMC (Gutzwiller) Chen & Liu (2026)
square 16x16, J = 0.8, Jd = 1 best variational -0.448881 ○ VMC (Transformer) Viteritti et al. (2025)
square 18x18, J = 0.8, Jd = 1 best variational -0.448859 ○ VMC (Transformer) Viteritti et al. (2025)
square 20x20, open, J = 0.8, Jd = 1 best variational -0.442928(3) VMC (PEPS) Liu et al. (2024)
square-tilted, 32 sites, J = 0.677, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.6772, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.67724, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.677244, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.677246, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.677248, Jd = 1 exact -0.375 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.6773, Jd = 1 exact -0.3750238 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.6775, Jd = 1 exact -0.3751152 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.6778, Jd = 1 exact -0.3752526 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.68, Jd = 1 exact -0.3762717 ED Sindermann et al. (2006)
square-tilted, 32 sites, J = 0.7, Jd = 1 exact -0.3867209 ED Sindermann et al. (2006)
Hubbard: 243 instances, energies as E/site
instance value energy method code
chain, 14 sites, U = 1, n ≈ 0.5714 exact -0.9116302 ED Wu et al. (2024) run script
best variational -0.9116293 (+9.1e-7) DMRG Wu et al. (2024) run script
best extrapolated -0.9116302(1) (−<1e-7) DMRG Wu et al. (2024) run script
chain, 14 sites, U = 1.66810054, n ≈ 0.5714 exact -0.8761535 ED Wu et al. (2024) run script
best variational -0.8761535 (+<1e-7) DMRG Wu et al. (2024) run script
best extrapolated -0.876153552(4) (−<1e-7) DMRG Wu et al. (2024) run script
chain, 14 sites, U = 2.15443469, n ≈ 0.5714 exact -0.8542284 ED Wu et al. (2024) run script
best variational -0.8542284 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 14 sites, U = 2.7825594, n ≈ 0.5714 exact -0.8300032 ED Wu et al. (2024) run script
best variational -0.8300032 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 14 sites, U = 3.59381366, n ≈ 0.5714 exact -0.804323 ED Wu et al. (2024) run script
best variational -0.804323 (+<1e-6) DMRG Wu et al. (2024) run script
chain, 14 sites, U = 4.64158882, n ≈ 0.5714 exact -0.7783541 ED QMBL check, checks/hubbard-u-labels/ QMBL code
best variational -0.7783541 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 14 sites, U = 4.64158883, n ≈ 0.5714 exact -0.7783541 ED Wu et al. (2024) run script
chain, 14 sites, U = 7.74263683, n ≈ 0.5714 exact -0.7304717 ED Wu et al. (2024) run script
best variational -0.7304717 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 14 sites, U = 10, n ≈ 0.5714 exact -0.7103639 ED Wu et al. (2024) run script
best variational -0.7103637 (+1.4e-7) DMRG Wu et al. (2024) run script
best extrapolated -0.71036386(2) (−<1e-7) DMRG Wu et al. (2024) run script
rectangular 10x16, open, U = 8, n = 0.875 best variational -0.7163(3) simple update (fPEPS) 10.1103/r4q9-4yvj
rectangular 10x16, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7434 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 12x16, open, U = 8, n = 0.875 best variational -0.72212 ○ VMC (transformer BF) Gu et al. (2026)
rectangular 12x16, U = 8, n = 0.875 best variational -0.7562 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 12x16, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.744 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 14x16, U = 8, n = 0.875 best variational -0.75830(4) VAFQMC Wu et al. (2024)
rectangular 16x32, U = 8, n = 0.875 best variational -0.7507 ○ VMC (SCALE) Gu et al. (2026) uses LaQX
best projected -0.7547 ○ FN-GFMC (SCALE) Gu et al. (2026)
rectangular 16x32, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7371 ○ VMC (SCALE) Gu et al. (2026) uses LaQX
best projected -0.7406 ○ FN-GFMC (SCALE) Gu et al. (2026)
rectangular 4x12, U = 8, n = 0.875 best variational -0.76608(1) VMC (HFPS) Chen et al. (2026) uses Quantax
rectangular 4x16, open, U = 8, n = 0.875 best variational -0.6853698 ○ DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
best extrapolated -0.68554(4) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
rectangular 4x16, U = 8, n = 0.875 best variational -0.76623(1) VMC (ACE) Gu et al. (2026) uses LaQX
best projected -0.76647(2) FN-GFMC (ACE) Gu et al. (2026)
best extrapolated -0.76748 ○ VMC (NNBF) Loehr & Clark (2025)
rectangular 4x16, periodic/open, U = 2, n = 0.8125 best variational -1.2852656 DMRG Wu et al. (2024) run script
rectangular 4x16, periodic/open, U = 8, n = 0.8125 best variational -0.853 DMRG Wu et al. (2024) run script
rectangular 4x16, periodic/open, U = 2, n = 0.875 best variational -1.2611875 DMRG Wu et al. (2024) run script
rectangular 4x16, periodic/open, U = 8, n = 0.875 best variational -0.7508328 DMRG Wu et al. (2024) run script
best extrapolated -0.75114(6) DMRG Wu et al. (2024) run script
rectangular 4x16, periodic/open, U = 2, n = 0.9375 best variational -1.2199062 DMRG Wu et al. (2024) run script
rectangular 4x16, periodic/open, U = 8, n = 0.9375 best variational -0.637875 DMRG Wu et al. (2024) run script
rectangular 4x16, periodic/open, U = 2, n = 1 best variational -1.1710781 DMRG Wu et al. (2024) run script
rectangular 4x16, periodic/open, U = 8, n = 1 best variational -0.5144219 DMRG Wu et al. (2024) run script
rectangular 4x24, U = 4, n ≈ 0.8333 best variational -1.07872(3) VMC (HFPS) Roth et al. (2025) uses Quantax
rectangular 4x8, U = 8, n = 0.875 best variational -0.768337(2) VMC (NNBF) Loehr & Clark (2025)
best extrapolated -0.768416 ○ VMC (NNBF) Loehr & Clark (2025)
rectangular 4x8, periodic/open, U = 8, n = 0.875 best variational -0.7363906 DMRG Wu et al. (2024) run script
best extrapolated -0.736431(9) DMRG Wu et al. (2024) run script
rectangular 6x16, open, U = 8, n = 0.875 best variational -0.70307 ○ VMC (transformer BF) Gu et al. (2026)
rectangular 6x16, U = 8, n = 0.875 best variational -0.7486 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x32, U = 8, n = 0.875 best variational -0.7483 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x40, U = 12, n = 0.875, t12 (t2 = -0.1) best variational -0.6206 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x40, U = 12, n = 0.875, t12 (t2 = -0.2) best variational -0.6187 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x40, U = 12, n = 0.875, t12 (t2 = -0.3) best variational -0.619 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x40, U = 12, n = 0.875, t12 (t2 = -0.35) best variational -0.6202 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x40, U = 12, n = 0.875, t12 (t2 = -0.4) best variational -0.622 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x40, U = 12, n = 0.875, t12 (t2 = -0.45) best variational -0.624 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x40, U = 12, n = 0.875, t12 (t2 = -0.5) best variational -0.626 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 8, n ≈ 0.8333 best variational -0.82075(3) VMC (Jastrow + BF) Wu et al. (2024) run script
best projected -0.82575(2) FN-GFMC (Jastrow + BF) Wu et al. (2024) run script
rectangular 6x48, U = 8, n = 0.875 best variational -0.74834(3) VMC (Jastrow + BF) Wu et al. (2024) run script
best projected -0.75398(2) FN-GFMC (Jastrow + BF) Wu et al. (2024) run script
rectangular 6x48, U = 12, n = 0.875 best variational -0.62556(3) VMC (Jastrow + BF) Wu et al. (2024) run script
best projected -0.63217(2) FN-GFMC (Jastrow + BF) Wu et al. (2024) run script
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = -0.1) best variational -0.6147 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = -0.2) best variational -0.6113 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = -0.3) best variational -0.6118 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = -0.35) best variational -0.6135 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = -0.4) best variational -0.6162 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = -0.45) best variational -0.6202 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = -0.5) best variational -0.6261 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = 0.1) best variational -0.6375 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = 0.15) best variational -0.6464 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = 0.2) best variational -0.6562 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 12, n = 0.875, t12 (t2 = 0.25) best variational -0.6669 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 6x48, U = 8, n ≈ 0.9167 best variational -0.67269(3) VMC (Jastrow + BF) Wu et al. (2024) run script
best projected -0.6862(2) CP-AFQMC (stripe) Xu et al. (2022)
rectangular 6x64, U = 8, n = 0.875 best variational -0.7482 ○ VMC (Jastrow + BF) Marino et al. (2022)
rectangular 8x10, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7427 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 8x12, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7456 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 8x16, open, U = 8, n = 0.875 best variational -0.71309 ○ VMC (transformer BF) Gu et al. (2026)
best extrapolated -0.718(1) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
rectangular 8x16, open, U = 8, n = 0.9375 best variational -0.6019(2) simple update (fPEPS) 10.1103/r4q9-4yvj
best extrapolated -0.6043(6) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
rectangular 8x16, U = 8, n = 0.875 best variational -0.7568 ○ VMC (tensor BF) Liang (2025)
rectangular 8x16, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7419 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 8x18, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7421 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 8x20, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7433 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 8x24, U = 8, n = 0.875 best variational -0.7546 ○ VMC (tensor BF) Liang (2025)
rectangular 8x24, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7423 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 8x32, U = 8, n = 0.875 best variational -0.7547 ○ VMC (tensor BF) Liang (2025)
rectangular 8x32, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.742 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
best extrapolated -0.7491 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
rectangular 8x48, U = 8, n ≈ 0.9167 best projected -0.6854(2) CP-AFQMC (stripe) Xu et al. (2022)
square 4x4, open, U = 8, n = 0.875 best variational -0.6326183 ○ DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
best extrapolated -0.6326190(1) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
square 4x4, open, U = 8, n = 1 best variational -0.4255259 ○ DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
best extrapolated -0.42552596(1) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
square 4x4, U = 0.1, n = 0.5 exact -1.2442068 ED Moreno et al. (2022)
best variational -1.2441738(2) (+3.3e-5) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 0.59948425, n = 0.5 exact -1.2171727 ED Moreno et al. (2022)
best variational -1.2171594(6) (+1.3e-5) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 1, n = 0.5 exact -1.1976241 ED Moreno et al. (2022)
best variational -1.197511(2) (+1.1e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 2, n = 0.5 exact -1.1559648 ED Wu et al. (2024) run script
best variational -1.1559648 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 2.15443469, n = 0.5 exact -1.1503325 ED Moreno et al. (2022)
best variational -1.148627(3) (+1.7e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 3.59381366, n = 0.5 exact -1.1061269 ED Moreno et al. (2022)
best variational -1.105848(3) (+2.8e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 3.5981, n = 0.5 exact -1.1060147 ED QMBL check, checks/hubbard-u-labels/ QMBL code
best variational -1.1060144 (+3.2e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 4, n = 0.5 exact -1.0959311 ED Wu et al. (2024) run script
best variational -1.095931 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 6, n = 0.5 exact -1.0562454 ED Wu et al. (2024) run script
best variational -1.0562454 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 7.74263683, n = 0.5 exact -1.0318222 ED Moreno et al. (2022)
best variational -1.031562(6) (+2.6e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 7.74264, n = 0.5 exact -1.0318221 ED QMBL check, checks/hubbard-u-labels/ QMBL code
best variational -1.0318221 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 8, n = 0.5 exact -1.0287892 ED Wu et al. (2024) run script
best variational -1.0287892 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 10, n = 0.5 exact -1.0089505 ED Wu et al. (2024) run script
best variational -1.0089505 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 2, n = 0.625 exact -1.3360594 ED Wu et al. (2024) run script
best variational -1.3360594 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 2.1544, n = 0.625 exact -1.325767 ED QMBL check, checks/hubbard-u-labels/ QMBL code
best variational -1.325767 (+<1e-6) DMRG Wu et al. (2024) run script
square 4x4, U = 2.15443469, n = 0.625 exact -1.3257647 ED Moreno et al. (2022)
best variational -1.3257435(1) (+2.1e-5) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 3.59381366, n = 0.625 exact -1.2432273 ED Moreno et al. (2022)
best variational -1.2431527(4) (+7.5e-5) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 3.5981, n = 0.625 exact -1.2430143 ED QMBL check, checks/hubbard-u-labels/ QMBL code
best variational -1.2430143 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 4, n = 0.625 exact -1.2238086 ED Wu et al. (2024) run script
best variational -1.2238086 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 6, n = 0.625 exact -1.1473978 ED Wu et al. (2024) run script
best variational -1.1473978 ○ (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 7.74263683, n = 0.625 exact -1.1002332 ED Moreno et al. (2022)
best variational -1.1001250(6) (+1.1e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, U = 7.74264, n = 0.625 exact -1.1002331 ED QMBL check, checks/hubbard-u-labels/ QMBL code
best variational -1.1002331 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 8, n = 0.625 exact -1.0943979 ED Wu et al. (2024) run script
best variational -1.0943979 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 10, n = 0.625 exact -1.0564725 ED Wu et al. (2024) run script
best variational -1.0564725 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, U = 8, n = 0.875 exact -0.7418022 ED QMBL check, checks/hubbard-4x4-n78-ed/ QMBL code
best variational -0.74177(5) (+3.2e-5) VMC (HFPS) Chen et al. (2026) uses Quantax
square 4x4, U = 2, n = 1 exact (stochastic) -1.1265(4) AFQMC Qin et al. (2016)
best variational -1.1248 ○ (+1.7e-3) VMC (HB) Zhou et al. (2026)
square 4x4, U = 4, n = 1 exact -0.8513659 ED QMBL check, checks/hubbard-4x4-half-filling-ed/ QMBL code
best variational -0.8511(1) (+2.3e-4) VMC (TQS) Yamazaki et al. (2026)
square 4x4, U = 6, n = 1 exact (stochastic) -0.6588(3) AFQMC Qin et al. (2016)
best variational -0.6577 ○ (+1.1e-3) VMC (HB) Zhou et al. (2026)
square 4x4, U = 8, n = 1 exact -0.5293047 ED QMBL check, checks/hubbard-4x4-half-filling-ed/ QMBL code
best variational -0.5292(3) (+1.1e-4) VMC (PITQS) Yamazaki et al. (2026) Zenodo 18334851
square 4x4, periodic/antiperiodic, U = 2, n = 1 exact (stochastic) -1.2571(1) AFQMC Qin et al. (2016)
best variational -1.25693(1) (+1.9e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, periodic/antiperiodic, U = 4, n = 1 exact (stochastic) -0.9121(2) AFQMC Qin et al. (2016)
best variational -0.9120(1) (+1.2e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, periodic/antiperiodic, U = 6, n = 1 exact (stochastic) -0.6814(4) AFQMC Qin et al. (2016)
best variational -0.68135(1) (+<1e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 4x4, periodic/antiperiodic, U = 8, n = 1 exact (stochastic) -0.5404(5) AFQMC Qin et al. (2016)
best variational -0.5401(1) (+2.8e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 6x6, open, U = 8, n ≈ 0.8889 best variational -0.6573063 ○ DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
best extrapolated -0.65768(8) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
square 6x6, open, U = 8, n ≈ 0.9444 best variational -0.5599001 ○ DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
best extrapolated -0.55997(2) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
square 6x6, U = 4, n ≈ 0.6667 best variational -1.1834(1) VAFQMC Levy et al. (2023)
best projected -1.18525(4) CP-AFQMC Shi & Zhang (2013)
square 6x6, U = 2, n = 1 exact (stochastic) -1.1516(1) AFQMC Qin et al. (2016)
best variational -1.1506 ○ (+9.8e-4) VMC (HB) Zhou et al. (2026)
square 6x6, U = 4, n = 1 exact (stochastic) -0.8574(3) AFQMC Qin et al. (2016)
best variational -0.8554 ○ (+2.0e-3) VMC (HB) Zhou et al. (2026)
square 6x6, U = 6, n = 1 exact (stochastic) -0.6594(3) AFQMC Qin et al. (2016)
square 6x6, U = 8, n = 1 exact (stochastic) -0.5278(6) AFQMC Qin et al. (2016)
best variational -0.5266 ○ (+1.2e-3) VMC (HB) Zhou et al. (2026)
square 6x6, U = 4, n ≈ 1.3333 best projected 0.14809(4) CP-AFQMC Shi & Zhang (2013)
square 6x6, periodic/antiperiodic, U = 2, n = 1 exact (stochastic) -1.20831(6) AFQMC Qin et al. (2016)
best variational -1.2079(1) (+4.1e-4) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 6x6, periodic/antiperiodic, U = 4, n = 1 exact (stochastic) -0.8731(6) AFQMC Qin et al. (2016)
best variational -0.87173(2) (+1.3e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 6x6, periodic/antiperiodic, U = 6, n = 1 exact (stochastic) -0.6622(3) AFQMC Qin et al. (2016)
best variational -0.66094(3) (+1.3e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 6x6, periodic/antiperiodic, U = 8, n = 1 exact (stochastic) -0.5281(3) AFQMC Qin et al. (2016)
best variational -0.52705(3) (+1.0e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square, 50 sites, U = 8, n = 0.84 best variational -0.82328(3) VAFQMC Wu et al. (2024)
square 8x8, open, U = 8, n = 0.875 best variational -0.69952 ○ VMC (transformer BF) Gu et al. (2026)
best extrapolated -0.704(1) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
square 8x8, open, U = 8, n ≈ 0.9688 best variational -0.5322603 ○ DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
best extrapolated -0.5335(3) DMRG 10.1103/r4q9-4yvj hczhai/2d-hubbard-dmrg-2024
square 8x8, U = 4, n = 0.4375 best projected -1.07180(2) CP-AFQMC Shi & Zhang (2013)
square 8x8, U = 4, n = 0.6875 best variational -1.1846 ○ VMC (tensor BF) Liang (2025)
best projected -1.1858(2) CP-AFQMC Shi & Zhang (2013)
square 8x8, U = -8, n ≈ 0.7813 exact (stochastic) -3.6258(1) AFQMC Wu et al. (2024) run scripts
square 8x8, U = -4, n ≈ 0.7813 exact (stochastic) -2.39630(9) AFQMC Wu et al. (2024) run scripts
square 8x8, U = 4, n ≈ 0.7813 best variational -1.13048(8) VAFQMC Levy et al. (2023)
best projected -1.13253(3) CP-AFQMC Levy et al. (2023)
square 8x8, U = 8, n ≈ 0.7813 best variational -0.91483(2) VMC (PP + RBM) Wu et al. (2024) run script
best projected -0.9252(1) CP-AFQMC Levy et al. (2023)
square 8x8, U = -8, n = 0.875 exact (stochastic) -4.01700(9) AFQMC Wu et al. (2024) run scripts
best variational -4.0169(1) (+1.0e-4) VMC (transformer BF) Viteritti et al. (2026)
best projected -4.0168 ○ (+2.0e-4) FN-GFMC (ACE) Gu et al. (2026)
square 8x8, U = -4, n = 0.875 exact (stochastic) -2.60123(8) AFQMC Wu et al. (2024) run scripts
square 8x8, U = -2, n = 0.875 exact (stochastic) -2.03430(7) DQMC Gu et al. (2026)
best variational -2.0338 ○ (+5.0e-4) VMC (ACE) Gu et al. (2026) uses LaQX
best projected -2.0339 ○ (+4.0e-4) FN-GFMC (ACE) Gu et al. (2026)
square 8x8, U = 4, n = 0.875 best variational -1.01391(8) VAFQMC Levy et al. (2023)
best projected -1.01923(6) CP-AFQMC Levy et al. (2023)
square 8x8, U = 8, n = 0.875 best variational -0.7532 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
best projected -0.7616(1) CP-AFQMC Levy et al. (2023)
square 8x8, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.75058(1) VMC (transformer BF) Viteritti et al. (2026)
best extrapolated -0.7540(4) VMC (transformer BF) Viteritti et al. (2026)
square 8x8, U = -8, n = 1 exact (stochastic) -4.52589(9) AFQMC Wu et al. (2024) run scripts
best variational -4.525834 † (+5.7e-5) VMC (HFPS) Chen et al. (2026) uses Quantax
square 8x8, U = -4, n = 1 exact (stochastic) -2.86037(6) AFQMC Wu et al. (2024) run scripts
best variational -2.859578 † (+8.0e-4) VMC (HFPS) Chen et al. (2026) uses Quantax
square 8x8, U = 2, n = 1 exact (stochastic) -1.16359(8) AFQMC Qin et al. (2016)
best variational -1.1626 ○ (+9.9e-4) VMC (HB) Zhou et al. (2026)
square 8x8, U = 4, n = 1 exact (stochastic) -0.86036(6) AFQMC Wu et al. (2024)
best variational -0.859156(8) (+1.2e-3) VMC (PP + RBM) Wu et al. (2024) run script
best projected -0.857653(9) (+2.7e-3) FN-GFMC (Jastrow + BF) Wu et al. (2024) run script
square 8x8, U = 6, n = 1 exact (stochastic) -0.6587(3) AFQMC Qin et al. (2016)
best variational -0.6554 ○ (+3.3e-3) VMC (HB) Zhou et al. (2026)
square 8x8, U = 8, n = 1 exact (stochastic) -0.52566(8) AFQMC Wu et al. (2024)
best variational -0.52459(1) (+1.1e-3) VMC (PP + RBM) Wu et al. (2024) run script
square 8x8, periodic/antiperiodic, U = 2, n = 1 exact (stochastic) -1.19231(5) AFQMC Qin et al. (2016)
best variational -1.19003(9) (+2.3e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 8x8, periodic/antiperiodic, U = 4, n = 1 exact (stochastic) -0.8642(2) AFQMC Qin et al. (2016)
best variational -0.8622(2) (+2.0e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 8x8, periodic/antiperiodic, U = 6, n = 1 exact (stochastic) -0.6589(3) AFQMC Qin et al. (2016)
best variational -0.6574(2) (+1.5e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 8x8, periodic/antiperiodic, U = 8, n = 1 exact (stochastic) -0.5259(3) AFQMC Qin et al. (2016)
best variational -0.5244(2) (+1.5e-3) VMC (HFDS) Moreno et al. (2022) uses NetKet
square 8x8, periodic/open, U = 8, n = 1 exact (stochastic) -0.5005(2) AFQMC Wu et al. (2024) run scripts
best variational -0.49944(4) (+1.0e-3) VAFQMC Wu et al. (2024)
best extrapolated -0.5000(3) (+4.1e-4) DMRG Wu et al. (2024) run script
square 10x10, U = 4, n = 0.8 best variational -1.11097(6) VAFQMC Levy et al. (2023)
best projected -1.1135(2) CP-AFQMC Shi & Zhang (2013)
square 10x10, U = 2, n = 1 exact (stochastic) -1.16908(4) AFQMC Qin et al. (2016)
best variational -1.1677 ○ (+1.4e-3) VMC (HB) Zhou et al. (2026)
square 10x10, U = 4, n = 1 exact (stochastic) -0.8612(4) AFQMC Qin et al. (2016)
best variational -0.8585 ○ (+2.7e-3) VMC (HB) Zhou et al. (2026)
square 10x10, U = 6, n = 1 exact (stochastic) -0.6580(2) AFQMC Qin et al. (2016)
best variational -0.655 ○ (+3.0e-3) VMC (HB) Zhou et al. (2026)
square 10x10, U = 8, n = 1 exact (stochastic) -0.5254(3) AFQMC Qin et al. (2016)
best variational -0.52492 ○ (+4.8e-4) VMC (transformer BF) Gu et al. (2026) bytedance/laqx
square 10x10, periodic/antiperiodic, U = 2, n = 1 exact (stochastic) -1.18505(4) AFQMC Qin et al. (2016)
square 10x10, periodic/antiperiodic, U = 4, n = 1 exact (stochastic) -0.8620(2) AFQMC Qin et al. (2016)
square 10x10, periodic/antiperiodic, U = 6, n = 1 exact (stochastic) -0.6576(2) AFQMC Qin et al. (2016)
square 10x10, periodic/antiperiodic, U = 8, n = 1 exact (stochastic) -0.5249(2) AFQMC Qin et al. (2016)
square 12x12, U = 4, n ≈ 0.8056 best variational -1.1061 ○ VMC (tensor BF) Liang (2025)
best projected -1.1089(2) CP-AFQMC Shi & Zhang (2013)
square 12x12, U = 2, n ≈ 0.8333 best variational -1.29500(3) VMC (HFPS) Roth et al. (2025) uses Quantax
square 12x12, U = 4, n ≈ 0.8333 best variational -1.0751(1) VMC (HFPS) Roth et al. (2025) uses Quantax
square 12x12, U = 6, n ≈ 0.8333 best variational -0.92516(5) VMC (HFPS) Roth et al. (2025) uses Quantax
square 12x12, U = 10, n ≈ 0.8333 best variational -0.76179(5) VMC (HFPS) Roth et al. (2025) uses Quantax
square 12x12, U = 15, n ≈ 0.8333 best variational -0.66690(5) VMC (HFPS) Roth et al. (2025) uses Quantax
square 12x12, U = -8, n = 0.875 best variational -4.0159 ○ VMC (ACE) Gu et al. (2026) uses LaQX
best projected -4.0161 ○ FN-GFMC (ACE) Gu et al. (2026)
square 12x12, U = -2, n = 0.875 exact (stochastic) -2.04160(5) DQMC Gu et al. (2026)
best variational -2.0405 ○ (+1.1e-3) VMC (ACE) Gu et al. (2026) uses LaQX
best projected -2.0407 ○ (+9.0e-4) FN-GFMC (ACE) Gu et al. (2026)
square 12x12, U = 8, n = 0.875 best variational -0.7567 ○ VMC (transformer BF) Gu et al. (2026) bytedance/laqx
square 12x12, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.74425(1) VMC (SBP) Rende et al. (2026)
square 12x12, U = 2, n = 1 exact (stochastic) -1.17187(5) AFQMC Qin et al. (2016)
square 12x12, U = 4, n = 1 exact (stochastic) -0.8608(1) AFQMC Qin et al. (2016)
square 12x12, U = 6, n = 1 exact (stochastic) -0.6574(1) AFQMC Qin et al. (2016)
square 12x12, U = 8, n = 1 exact (stochastic) -0.5246(1) AFQMC Qin et al. (2016)
best variational -0.5244 ○ (+1.8e-4) VMC (transformer BF) Gu et al. (2026) bytedance/laqx
square 12x12, periodic/antiperiodic, U = 2, n = 1 exact (stochastic) -1.18133(2) AFQMC Qin et al. (2016)
square 12x12, periodic/antiperiodic, U = 4, n = 1 exact (stochastic) -0.8610(2) AFQMC Qin et al. (2016)
square 12x12, periodic/antiperiodic, U = 6, n = 1 exact (stochastic) -0.6574(1) AFQMC Qin et al. (2016)
square 12x12, periodic/antiperiodic, U = 8, n = 1 exact (stochastic) -0.5249(2) AFQMC Qin et al. (2016)
best variational -0.5224 ○ (+2.5e-3) VMC (tensor BF) Liang (2025)
square 14x14, U = 2, n = 1 exact (stochastic) -1.17337(3) AFQMC Qin et al. (2016)
square 14x14, U = 4, n = 1 exact (stochastic) -0.8606(1) AFQMC Qin et al. (2016)
square 14x14, U = 6, n = 1 exact (stochastic) -0.6569(1) AFQMC Qin et al. (2016)
square 14x14, U = 8, n = 1 exact (stochastic) -0.5247(2) AFQMC Qin et al. (2016)
square 14x14, periodic/antiperiodic, U = 2, n = 1 exact (stochastic) -1.17926(2) AFQMC Qin et al. (2016)
square 14x14, periodic/antiperiodic, U = 4, n = 1 exact (stochastic) -0.8607(2) AFQMC Qin et al. (2016)
square 14x14, periodic/antiperiodic, U = 6, n = 1 exact (stochastic) -0.6570(2) AFQMC Qin et al. (2016)
square 14x14, periodic/antiperiodic, U = 8, n = 1 exact (stochastic) -0.5246(2) AFQMC Qin et al. (2016)
square 16x16, open, U = 8, n = 0.875 best variational -0.728 ○ VMC (ACE) Gu et al. (2026) uses LaQX
best projected -0.7288 ○ FN-GFMC (ACE) Gu et al. (2026)
square 16x16, open, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.7097(1) VMC (tensor BF) Liang (2026)
square 16x16, U = 8, n ≈ 0.8281 best variational -0.83788(6) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.8438 best variational -0.81198(6) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.8516 best variational -0.79896(5) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.8594 best variational -0.78530(6) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.8672 best variational -0.77196(6) VAFQMC Wu et al. (2024)
square 16x16, U = -8, n = 0.875 exact (stochastic) -4.01629(5) AFQMC Wu et al. (2024) run scripts
square 16x16, U = -4, n = 0.875 exact (stochastic) -2.60067(6) AFQMC Wu et al. (2024) run scripts
square 16x16, U = 4, n = 0.875 best variational -1.02916(2) VAFQMC Wu et al. (2024)
square 16x16, U = 6, n = 0.875 best variational -0.86592(2) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n = 0.875 best variational -0.75865(3) VAFQMC Wu et al. (2024)
best projected -0.7583 ○ FN-GFMC (ACE) Gu et al. (2026)
square 16x16, U = 8, n = 0.875, t12 (t2 = -0.1) best variational -0.7370(1) VMC (HFPS) Roth et al. (2025) uses Quantax
square 16x16, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.74411(1) VMC (SBP) Rende et al. (2026)
best projected -0.744 ○ FN-GFMC (ACE) Gu et al. (2026)
square 16x16, U = 8, n = 0.875, t12 (t2 = -0.3) best variational -0.7375(1) VMC (HFPS) Roth et al. (2025) uses Quantax
square 16x16, U = 8, n ≈ 0.8828 best variational -0.74455(3) VAFQMC Wu et al. (2024)
square 16x16, U = 4, n ≈ 0.8906 best variational -1.00849(2) VAFQMC Wu et al. (2024)
square 16x16, U = 6, n ≈ 0.8906 best variational -0.84058(2) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.8906 best variational -0.73038(5) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.8984 best variational -0.71584(5) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.9063 best variational -0.70135(3) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.9141 best variational -0.68678(5) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n ≈ 0.9219 best variational -0.67215(5) VAFQMC Wu et al. (2024)
square 16x16, U = 8, n = 0.9375 best variational -0.64053(5) VAFQMC Wu et al. (2024)
square 16x16, U = -8, n = 1 exact (stochastic) -4.52446(6) AFQMC Wu et al. (2024) run scripts
square 16x16, U = -4, n = 1 exact (stochastic) -2.8605(1) AFQMC Wu et al. (2024) run scripts
square 16x16, U = 2, n = 1 exact (stochastic) -1.17420(2) AFQMC Qin et al. (2016)
square 16x16, U = 4, n = 1 exact (stochastic) -0.8605(2) AFQMC Qin et al. (2016)
square 16x16, U = 6, n = 1 exact (stochastic) -0.6570(1) AFQMC Qin et al. (2016)
square 16x16, U = 8, n = 1 exact (stochastic) -0.5243(1) AFQMC Qin et al. (2016)
square 16x16, periodic/antiperiodic, U = 8, n ≈ 0.8359 best variational -0.82333(3) VAFQMC Wu et al. (2024)
square 16x16, periodic/antiperiodic, U = 8, n ≈ 0.8359, t12 (t2 = -0.25) best variational -0.79937(4) VMC (PP + RBM) Wu et al. (2024) run script
square 16x16, periodic/antiperiodic, U = 8, n ≈ 0.8359, t12 (t2 = -0.25), UV1V2 best variational 1.25918(3) VMC (PP + RBM) Wu et al. (2024) run script
square 16x16, periodic/antiperiodic, U = 2, n = 1 exact (stochastic) -1.17798(2) AFQMC Qin et al. (2016)
square 16x16, periodic/antiperiodic, U = 4, n = 1 exact (stochastic) -0.8605(2) AFQMC Qin et al. (2016)
square 16x16, periodic/antiperiodic, U = 6, n = 1 exact (stochastic) -0.6571(2) AFQMC Qin et al. (2016)
square 16x16, periodic/antiperiodic, U = 8, n = 1 exact (stochastic) -0.5244(1) AFQMC Qin et al. (2016)
best variational -0.52427(4) (+1.5e-4) VAFQMC Wu et al. (2024)
square, 288 sites, U = 2, n ≈ 0.8333 best variational -1.29563(3) VMC (HFPS) Roth et al. (2025) uses Quantax
square, 288 sites, U = 4, n ≈ 0.8333 best variational -1.07256(5) VMC (HFPS) Roth et al. (2025) uses Quantax
square, 288 sites, U = 6, n ≈ 0.8333 best variational -0.91859(6) VMC (HFPS) Roth et al. (2025) uses Quantax
square 20x20, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.74382(1) VMC (SBP) Rende et al. (2026)
square 24x24, U = 8, n = 0.875, t12 (t2 = -0.2) best variational -0.74397(1) VMC (SBP) Rende et al. (2026)
square 32x32, U = 8, n = 0.875 best variational -0.7501 ○ VMC (SCALE) Gu et al. (2026) uses LaQX
best projected -0.7548 ○ FN-GFMC (SCALE) Gu et al. (2026)
square, infinite lattice, U = 2, n = 0.8 best extrapolated -1.306(2) CP-AFQMC LeBlanc et al. (2015)
best approximate -1.3062(4) DMET LeBlanc et al. (2015)
square, infinite lattice, U = 2, n = 0.875 best extrapolated -1.270(2) FN-DMC LeBlanc et al. (2015)
best approximate -1.2721(6) DMET LeBlanc et al. (2015)
square, infinite lattice, U = 2, n = 1 best extrapolated -1.1763(2) AFQMC LeBlanc et al. (2015)
best approximate -1.1764(3) DMET LeBlanc et al. (2015)
square, infinite lattice, U = 4, n = 0.3 best extrapolated -0.8793(2) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 4, n = 0.5 best extrapolated -1.141(2) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 4, n = 0.6 best extrapolated -1.1845(5) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 4, n = 0.75 best extrapolated -1.1491(2) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 4, n = 0.8 best extrapolated -1.110(3) CP-AFQMC LeBlanc et al. (2015)
best approximate -1.108(2) DMET LeBlanc et al. (2015)
square, infinite lattice, U = 4, n = 0.875 best extrapolated -1.032(1) CP-AFQMC Qin et al. (2016)
best approximate -1.031(3) DMET LeBlanc et al. (2015)
square, infinite lattice, U = 4, n = 1 best extrapolated -0.8605(5) DMRG LeBlanc et al. (2015)
best approximate -0.861 ○ UCCSDTQ* LeBlanc et al. (2015)
square, infinite lattice, U = 6, n = 0.8 best extrapolated -0.967(1) FN-DMC LeBlanc et al. (2015)
best approximate -0.977(4) DMET LeBlanc et al. (2015)
square, infinite lattice, U = 6, n = 0.875 best extrapolated -0.854(2) FN-DMC LeBlanc et al. (2015)
best approximate -0.8767(7) DMET Zheng et al. (2017)
square, infinite lattice, U = 6, n = 1 best extrapolated -0.6568(3) AFQMC LeBlanc et al. (2015)
best approximate -0.6582 ○ UCCSDTQ* LeBlanc et al. (2015)
square, infinite lattice, U = 8, n = 0.3 best extrapolated -0.8534(1) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 8, n = 0.5 best extrapolated -1.066(2) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 8, n = 0.6 best extrapolated -1.0729(1) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 8, n = 0.75 best extrapolated -0.9666(4) CP-AFQMC Qin et al. (2016)
square, infinite lattice, U = 8, n = 0.8 best extrapolated -0.877(1) FN-DMC LeBlanc et al. (2015)
best approximate -0.88(3) DMET LeBlanc et al. (2015)
square, infinite lattice, U = 8, n = 0.875 best extrapolated -0.773(1) CP-AFQMC Qin et al. (2016)
best approximate -0.77063(1) DMET Zheng et al. (2017)
square, infinite lattice, U = 8, n = 1 best extrapolated -0.5247(2) AFQMC LeBlanc et al. (2015)
best approximate -0.5255 ○ UCCSDTQ* LeBlanc et al. (2015)
square, infinite lattice, U = 12, n = 0.875 best approximate -0.6531(1) DMET Zheng et al. (2017)
square, infinite lattice, U = 12, n = 1 best extrapolated -0.3693(2) AFQMC LeBlanc et al. (2015)
best approximate -0.3696 ○ UCCSDTQ* LeBlanc et al. (2015)
Spinless t-V: 14 instances, energies as E/site
instance value energy method code
chain, 32 sites, V = 1, n = 0.5 exact -0.498339 ED run script, Wu et al. (2024)
best variational -0.498339 (+<1e-6) DMRG Wu et al. (2024) run script
chain, 32 sites, V = 2, n = 0.5 exact -0.3852719 ED run script, Wu et al. (2024)
best variational -0.3852719 ○ (+<1e-7) DMRG Wu et al. (2024) run script
chain, 32 sites, V = 4, n = 0.5 exact -0.2344426 ED run script, Wu et al. (2024)
best variational -0.2344426 ○ (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, V = 0.01, n = 0.3125 exact -0.7487516 ED Wu et al. (2024) run script
best variational -0.7487521(6) (−4.2e-7) VMC (SJ + RBM) Wu et al. (2024) run script
square 4x4, V = 0.1, n = 0.3125 exact -0.7376632 ED Wu et al. (2024) run script
best variational -0.7376632(3) (−<1e-7) VMC (SJB + RBM) Wu et al. (2024) run script
square 4x4, V = 1, n = 0.3125 exact -0.6400407 ED Wu et al. (2024) run script
best variational -0.6400407 (+<1e-7) DMRG Wu et al. (2024) run script
square 4x4, V = 10, n = 0.3125 exact -0.2532535 ED Wu et al. (2024) run script
best variational -0.2532535 (−<1e-7) DMRG Wu et al. (2024) run script
square 6x6, V = 0.01, n ≈ 0.3611 exact -0.7759279 ED Humeniuk et al. (2022) uses QuSpin
best variational -0.7759280(1) (−<1e-7) VMC (SJ + RBM) Wu et al. (2024) run script
square 6x6, V = 0.1, n ≈ 0.3611 exact -0.7594596 ED Humeniuk et al. (2022) uses QuSpin
best variational -0.759460(1) (−2.4e-7) VMC (SJ + RBM) Wu et al. (2024) run script
square 6x6, V = 1, n ≈ 0.3611 exact -0.6132603 ED Humeniuk et al. (2022) uses QuSpin
best variational -0.6132263 (+3.4e-5) DMRG Wu et al. (2024) run script
square 6x6, V = 10, n ≈ 0.3611 exact -0.220223 ED Humeniuk et al. (2022) uses QuSpin
best variational -0.2201239 (+9.9e-5) DMRG Wu et al. (2024) run script
square 8x8, V = 1, n = 0.5 exact (stochastic) -0.4607(4) CT-QMC Wu et al. (2024) run script
best variational -0.4590635 (+1.6e-3) DMRG Wu et al. (2024) run script
square 8x8, V = 2, n = 0.5 exact (stochastic) -0.292(1) CT-QMC Wu et al. (2024) run script
best variational -0.2911555 (+1.2e-3) DMRG Wu et al. (2024) run script
square 8x8, V = 4, n = 0.5 best variational -0.1601344 DMRG Wu et al. (2024) run script
t-J: 27 instances, energies as E/site
instance value energy method code
honeycomb-flake24, 24 sites, open, J = 0.333333, 1 hole exact -0.3441916 ED Cui et al. (2024)
best variational -0.3366806 ○ (+7.5e-3) VMC (phase string) Cui et al. (2024)
honeycomb-flake24, 24 sites, open, J = 0.333333, 2 holes exact -0.4143583 ED Cui et al. (2024)
best variational -0.398 ○ (+1.6e-2) VMC (phase string) Cui et al. (2024)
ladder 2x11, J = 0.5, 2 holes exact -0.5908993 ED Chiappa et al. (2001)
ladder 2x13, J = 0.5, 2 holes exact -0.5733713 ED Chiappa et al. (2001)
ladder 3x6, antiperiodic legs, J = 0.5, 1 hole exact -0.5781986 ED Rice et al. (1997)
ladder 3x6, antiperiodic legs, J = 0.5, 2 holes exact -0.6559335 ED Rice et al. (1997)
rectangular 6x16, periodic/open, J = 0.35, 8 holes best variational -0.5470833 ○ DMRG McCulloch et al. (2001)
best extrapolated -0.5484(5) DMRG McCulloch et al. (2001)
square 4x4, open, J = 0.4, 2 holes exact -0.5643668 ED Dong et al. (2020)
best variational -0.56428(2) (+8.7e-5) VMC (fPEPS) Dong et al. (2020)
square, 18 sites, J = 0.4, 2 holes exact -0.6590431 ED Becca et al. (2001)
best variational -0.65904 (+3.1e-6) VMC (Gutzwiller) Becca et al. (2001)
square, 26 sites, J = 0.3, 2 holes exact -0.5009718 ED Lugas et al. (2006)
best variational -0.48476(1) (+1.6e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -0.49445(2) (+6.5e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 0.4, 2 holes exact -0.5945167 ED Lugas et al. (2006)
best variational -0.57978(1) (+1.5e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -0.58881(2) (+5.7e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 0.5, 2 holes exact -0.6894488 ED Lugas et al. (2006)
best variational -0.67568(1) (+1.4e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -0.68434(3) (+5.1e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 0.6, 2 holes exact -0.7853745 ED Lugas et al. (2006)
best variational -0.77228(1) (+1.3e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -0.78062(3) (+4.8e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 0.8, 2 holes exact -0.9793539 ED Lugas et al. (2006)
best variational -0.96706(1) (+1.2e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -0.97505(3) (+4.3e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 1, 2 holes exact -1.1753789 ED Lugas et al. (2006)
best variational -1.16352(1) (+1.2e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -1.17136(2) (+4.0e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 0.3, 4 holes exact -0.6426164 ED D. Poilblanc (unpublished), quoted in Sorella (2001)
best variational -0.6387(1) (+3.9e-3) VMC (Gutzwiller) Sorella (2001)
best projected -0.6371(1) (+5.5e-3) FN-GFMC (Gutzwiller) Sorella (2001)
square, 26 sites, J = 0.4, 4 holes exact -0.7143669 ED Lugas et al. (2006)
best variational -0.68946(1) (+2.5e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -0.70292(2) (+1.1e-2) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 0.5, 4 holes exact -0.7881242 ED D. Poilblanc (unpublished), quoted in Sorella (2001)
best variational -0.7855(1) (+2.6e-3) VMC (Gutzwiller) Sorella (2001)
best projected -0.7841(1) (+4.0e-3) FN-GFMC (Gutzwiller) Sorella (2001)
square, 26 sites, J = 0.6, 4 holes exact -0.8633713 ED Lugas et al. (2006)
best variational -0.84170(1) (+2.2e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -0.85348(3) (+9.9e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 0.8, 4 holes exact -1.0173302 ED Lugas et al. (2006)
best variational -0.99709(1) (+2.0e-2) VMC (Pfaffian) Lugas et al. (2006)
best projected -1.00806(2) (+9.3e-3) FN-GFMC (Pfaffian) Lugas et al. (2006)
square, 26 sites, J = 1, 4 holes exact -1.1749259 ED D. Poilblanc (unpublished), quoted in Sorella (2001)
best variational -1.1724(1) (+2.5e-3) VMC (Gutzwiller) Sorella (2001)
best projected -1.1706(1) (+4.3e-3) FN-GFMC (Gutzwiller) Sorella (2001)
square, 32 sites, J = 0.3, t′ = 0.3, t″ = -0.2, 1 hole exact -0.4348005 ED Leung (2006)
square, 32 sites, J = 0.3, t′ = 0.3, t″ = -0.2, 2 holes exact -0.5188028 ED Leung (2006)
square, 32 sites, J = 0.3, t′ = 0.3, t″ = -0.2, 4 holes exact -0.6394265 ED Leung (2006)
square 8x8, open, J = 0.333333, 1 hole best variational -0.380099 ○ DMRG Cui et al. (2026)
square 8x8, J = 0.2, 14 holes best variational -0.685(1) Power-Lanczos Shih et al. (2001)
best extrapolated -0.690(5) Power-Lanczos Shih et al. (2001)
square 8x8, J = 0.4, 8 holes best variational -0.64266(8) VMC (Gutzwiller) Sorella et al. (2002)
best projected -0.66672(6) FN-GFMC (Gutzwiller) Sorella et al. (2002)
best extrapolated -0.671(1) VMC (Gutzwiller) Sorella et al. (2002)
Transverse-field Ising: 12 instances, energies as E/N (Pauli)
instance value energy method code
chain, 10 sites, open, h = 1 exact -1.238149 ED Wu et al. (2024) run script
best variational -1.238149 (−<1e-6) DMRG Wu et al. (2024) run script
chain, 10 sites, h = 1 exact -1.2784906 Exact solution Wu et al. (2024) run script
best variational -1.2784906 (−<1e-7) DMRG Wu et al. (2024) run script
chain, 32 sites, h = 0.5 exact -1.0635444 Exact solution Wu et al. (2024) run script
best variational -1.0635444 (+<1e-7) DMRG Wu et al. (2024) run script
chain, 32 sites, h = 1 exact -1.273751 Exact solution Wu et al. (2024) run script
best variational -1.273751 (+<1e-6) DMRG Wu et al. (2024) run script
square 6x6, h = 3 exact -3.2009085 ED Wu et al. (2024) run script
best variational -3.2009084 (+1.6e-7) DMRG Wu et al. (2024) run script
square 8x8, open, h = 3 best variational -3.1641828 ○ DMRG Dao (2026)
square 10x10, open, h = 3 best variational -3.16977 ○ DMRG Dao (2026)
square 12x12, open, h = 2 best variational -2.4096026 ○ DMRG Hibat-Allah et al. (2020)
square 12x12, open, h = 3 best variational -3.1739018(2) VMC (2D RNN) Hibat-Allah et al. (2020) run script
square 12x12, open, h = 4 best variational -4.1217979 ○ DMRG Hibat-Allah et al. (2020)
square 20x20, open, h = 3 best variational -3.18197 ○ DMRG Ganahl et al. (2023)
square, infinite lattice, h = 3.04438 best variational -3.2342607 ○ iPEPS Rader & Läuchli (2018)
best extrapolated -3.2342623 ○ iPEPS Rader & Läuchli (2018)
Impurity: 12 instances, energies as E (total)
instance value energy method code
SB-DMFT-MI-HF, size 10 exact -34.5805205 ED run script, Wu et al. (2024)
best variational -34.5805205 (+<1e-7) DMRG run script, Wu et al. (2024)
SB-DMFT-MT-AHF, size 9 exact -13.8893249 ED run script, Wu et al. (2024)
best variational -13.8893249 (+<1e-7) DMRG Wu et al. (2024) run script
SB-DMFT-MT-HF, size 9 exact -23.3009472 ED run script, Wu et al. (2024)
best variational -23.3009472 (+<1e-7) DMRG Wu et al. (2024) run script
SB-IMP, size 9 exact -10.4871285 ED run script, Wu et al. (2024)
best variational -10.4871285 (+<1e-7) DMRG Wu et al. (2024) run script
TB-DMFT, size 9 best variational -112.9042852 DMRG Wu et al. (2024) run script
TB-DMFT, size 19 best variational -224.3360713 DMRG Wu et al. (2024) run script
TB-DMFT, size 119 best variational -1307.5645417 DMRG Wu et al. (2024) run script
TB-DMFT, size 309 best variational -3378.6762368 DMRG Wu et al. (2024) run script
TB-DMFT-SOC, size 9 best variational -112.8717703 DMRG Wu et al. (2024) run script
TB-DMFT-SOC, size 19 best variational -219.766911 DMRG Wu et al. (2024) run script
TB-DMFT-SOC, size 119 best variational -1305.3902308 DMRG Wu et al. (2024) run script
TB-DMFT-SOC, size 309 best variational -3351.7573592 DMRG Wu et al. (2024) run script
Electron gas, 3D: 249 instances, energies as E/N (Ha)
instance value energy method code
bcc cell, N = 27, rs = 0.2, polarized best variational 44.18067(2) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected 44.18224(1) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 0.5, polarized best variational 6.318704(2) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected 6.319754(7) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 1, polarized best variational 1.261547(1) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected 1.261975(2) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 10, polarized best variational -0.050320(5) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.0503349(8) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 2, polarized best variational 0.152086(1) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected 0.152077(4) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 3, polarized best variational -0.006961(2) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.006966(2) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 30, polarized best variational -0.022541(5) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.0225620(2) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 5, polarized best variational -0.057691(4) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.057702(1) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 50, polarized best variational -0.014478(4) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.0144918(1) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 70, polarized best variational -0.010693(3) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.0107118(1) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 27, rs = 90, polarized best variational -0.008496(1) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.0085137(2) FN-DMC (SJB) Cassella et al. (2023) uses CASINO
bcc cell, N = 64, rs = 100, unpolarized best variational -0.00767129(8) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0076974(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 64, rs = 125, unpolarized best variational -0.0062378(1) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0062597(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 64, rs = 80, unpolarized best variational -0.0093993(3) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0094484(2) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 64, rs = 90, unpolarized best variational -0.00844873(6) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0084813(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 64, rs = 100, polarized best variational -0.0076803(2) VMC (SJB) Azadi & Drummond (2022) uses CASINO
best projected -0.00769619(9) FN-DMC Azadi & Drummond (2022) uses CASINO
bcc cell, N = 64, rs = 125, polarized best variational -0.00624309(3) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0062592(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 64, rs = 80, polarized best variational -0.0094086(1) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.00944340(6) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 64, rs = 90, polarized best variational -0.00845026(5) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.00847899(9) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 100, unpolarized best variational -0.00765917(9) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0076828(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 125, unpolarized best variational -0.00623503(4) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.00624956(9) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 80, unpolarized best variational -0.0093763(1) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0094299(3) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 90, unpolarized best variational -0.00843572(7) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0084658(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 100, polarized best variational -0.0076584(2) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0076816(4) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 125, polarized best variational -0.00623504(4) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.00624968(7) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 80, polarized best variational -0.00939055(8) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0094277(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 216, rs = 90, polarized best variational -0.00843484(6) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0084646(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 100, unpolarized best variational -0.00765566(9) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0076790(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 125, unpolarized best variational -0.00623185(4) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.00624652(5) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 80, unpolarized best variational -0.0093843(1) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0094232(2) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 90, unpolarized best variational -0.00843112(8) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0084611(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 100, polarized best variational -0.0076578(4) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0076795(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 125, polarized best variational -0.00623263(4) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.00624666(6) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 80, polarized best variational -0.00938865(8) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.00942260(9) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
bcc cell, N = 512, rs = 90, polarized best variational -0.00843318(7) VMC (SJ) Azadi & Drummond (2022) uses CASINO
best projected -0.0084605(1) FN-DMC (SJ) Azadi & Drummond (2022) uses CASINO
fcc cell, N = 54, rs = 2, unpolarized best projected 0.00426(2) FN-DMC Gurtubay et al. (2010) uses CASINO 2.1.400
fcc cell, N = 102, rs = 2, unpolarized best projected 0.00081(2) FN-DMC Gurtubay et al. (2010) uses CASINO 2.1.400
fcc cell, N = 130, rs = 100, unpolarized best variational -0.0076434(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00767914(4) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 130, rs = 30, unpolarized best variational -0.0225999(8) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0226541(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 130, rs = 40, unpolarized best variational -0.0175766(8) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01762938(7) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 130, rs = 50, unpolarized best variational -0.0143571(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144253(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 130, rs = 60, unpolarized best variational -0.0122189(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01226761(6) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 130, rs = 70, unpolarized best variational -0.0105888(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106437(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 130, rs = 80, unpolarized best variational -0.0093925(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00943534(6) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 136, rs = 30, N↑ = 85, N↓ = 51 best variational -0.0224390(7) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0225752(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 136, rs = 40, N↑ = 85, N↓ = 51 best variational -0.0174776(5) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175820(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 136, rs = 50, N↑ = 85, N↓ = 51 best variational -0.0143356(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144239(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 136, rs = 60, N↑ = 85, N↓ = 51 best variational -0.0121693(5) VMC (SJ) Azadi & Drummond (2022)
best projected -0.01224281(8) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 136, rs = 70, N↑ = 85, N↓ = 51 best variational -0.0105784(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.01064357(8) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 136, rs = 80, N↑ = 85, N↓ = 51 best variational -0.0093583(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.00941978(8) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 137, rs = 100, polarized best variational -0.0076530(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00767943(5) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 137, rs = 30, polarized best variational -0.0224803(7) VMC (SJB) Azadi & Drummond (2022)
best projected -0.02251468(9) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 137, rs = 40, polarized best variational -0.0175368(5) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01757424(6) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 137, rs = 50, polarized best variational -0.0143754(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144184(3) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 137, rs = 60, polarized best variational -0.0122233(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01225634(5) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 137, rs = 70, polarized best variational -0.0106119(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106489(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 137, rs = 80, polarized best variational -0.0094043(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00943313(4) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 140, rs = 100, N↑ = 105, N↓ = 35 best variational -0.0076402(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00767946(6) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 140, rs = 30, N↑ = 105, N↓ = 35 best variational -0.0225221(6) VMC (SJB) Azadi & Drummond (2022)
best projected -0.02262347(5) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 140, rs = 40, N↑ = 105, N↓ = 35 best variational -0.0175382(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01761925(4) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 140, rs = 50, N↑ = 105, N↓ = 35 best variational -0.0143415(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144259(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 140, rs = 60, N↑ = 105, N↓ = 35 best variational -0.0122063(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01226566(4) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 140, rs = 70, N↑ = 105, N↓ = 35 best variational -0.0105822(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106464(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 140, rs = 80, N↑ = 105, N↓ = 35 best variational -0.0093864(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00943526(5) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 152, rs = 30, N↑ = 133, N↓ = 19 best variational -0.0224543(6) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0225363(3) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 152, rs = 40, N↑ = 133, N↓ = 19 best variational -0.0175016(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175731(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 152, rs = 50, N↑ = 133, N↓ = 19 best variational -0.0143617(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144243(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 152, rs = 60, N↑ = 133, N↓ = 19 best variational -0.0121888(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0122460(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 152, rs = 70, N↑ = 133, N↓ = 19 best variational -0.0105960(2) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106479(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 152, rs = 80, N↑ = 133, N↓ = 19 best variational -0.0093769(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0094245(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 169, rs = 30, polarized best variational -0.0224527(6) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0224795(5) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 169, rs = 40, polarized best variational -0.0175196(5) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175515(3) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 169, rs = 50, polarized best variational -0.0143793(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144154(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 169, rs = 60, polarized best variational -0.0122080(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0122425(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 169, rs = 70, polarized best variational -0.0106158(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106470(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 169, rs = 80, polarized best variational -0.0093933(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0094248(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 178, rs = 100, unpolarized best variational -0.0076356(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00767661(9) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 178, rs = 2, unpolarized best projected 0.00892(2) FN-DMC Gurtubay et al. (2010) uses CASINO 2.1.400
fcc cell, N = 178, rs = 30, unpolarized best variational -0.0225404(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0226461(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 178, rs = 40, unpolarized best variational -0.0175445(6) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01762589(7) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 178, rs = 50, unpolarized best variational -0.0143317(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144184(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 178, rs = 60, unpolarized best variational -0.0122063(5) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01226479(7) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 178, rs = 70, unpolarized best variational -0.0105749(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106391(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 178, rs = 80, unpolarized best variational -0.0093822(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00943287(9) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 181, rs = 100, polarized best variational -0.0076512(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0076780(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 181, rs = 30, polarized best variational -0.0224736(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0225066(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 181, rs = 40, polarized best variational -0.0175354(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01756983(5) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 181, rs = 50, polarized best variational -0.0143712(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144139(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 181, rs = 60, polarized best variational -0.0122180(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01225212(6) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 181, rs = 70, polarized best variational -0.0106097(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106461(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 181, rs = 80, polarized best variational -0.0094012(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00943101(6) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 30, N↑ = 115, N↓ = 69 best variational -0.0224577(6) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0225651(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 40, N↑ = 115, N↓ = 69 best variational -0.0174818(5) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175749(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 50, N↑ = 115, N↓ = 69 best variational -0.0143354(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144186(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 60, N↑ = 115, N↓ = 69 best variational -0.0121663(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0122379(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 70, N↑ = 115, N↓ = 69 best variational -0.0105739(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.01064014(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 80, N↑ = 115, N↓ = 69 best variational -0.0093549(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.00941649(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 30, N↑ = 161, N↓ = 23 best variational -0.0224608(5) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0225319(3) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 40, N↑ = 161, N↓ = 23 best variational -0.0175027(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175701(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 50, N↑ = 161, N↓ = 23 best variational -0.0143616(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144220(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 60, N↑ = 161, N↓ = 23 best variational -0.0121877(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0122440(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 70, N↑ = 161, N↓ = 23 best variational -0.0105942(2) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106463(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 184, rs = 80, N↑ = 161, N↓ = 23 best variational -0.0093734(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0094229(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 188, rs = 100, N↑ = 141, N↓ = 47 best variational -0.0076410(1) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00767704(8) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 188, rs = 30, N↑ = 141, N↓ = 47 best variational -0.0225381(5) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0226138(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 188, rs = 40, N↑ = 141, N↓ = 47 best variational -0.0175518(5) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01761386(6) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 188, rs = 50, N↑ = 141, N↓ = 47 best variational -0.0143414(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144203(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 188, rs = 60, N↑ = 141, N↓ = 47 best variational -0.0122054(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01226154(7) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 188, rs = 70, N↑ = 141, N↓ = 47 best variational -0.0105783(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106423(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 188, rs = 80, N↑ = 141, N↓ = 47 best variational -0.0093829(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.00943141(9) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 216, rs = 30, N↑ = 189, N↓ = 27 best variational -0.0224319(5) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0225259(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 216, rs = 40, N↑ = 189, N↓ = 27 best variational -0.0174868(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175662(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 216, rs = 50, N↑ = 189, N↓ = 27 best variational -0.0143535(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144192(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 216, rs = 60, N↑ = 189, N↓ = 27 best variational -0.0121833(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0122417(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 216, rs = 70, N↑ = 189, N↓ = 27 best variational -0.0105860(2) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106436(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 216, rs = 80, N↑ = 189, N↓ = 27 best variational -0.0093712(2) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0094211(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 226, rs = 100, unpolarized best variational -0.0076375(1) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0076755(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 226, rs = 2, unpolarized best projected 0.00202(2) FN-DMC Gurtubay et al. (2010) uses CASINO 2.1.400
fcc cell, N = 226, rs = 30, unpolarized best variational -0.0225531(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0226358(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 226, rs = 40, unpolarized best variational -0.0175548(6) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01762088(9) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 226, rs = 50, unpolarized best variational -0.0143403(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144151(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 226, rs = 60, unpolarized best variational -0.0122056(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0122608(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 226, rs = 70, unpolarized best variational -0.0105783(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106371(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 226, rs = 80, unpolarized best variational -0.0093862(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0094307(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 229, rs = 100, polarized best variational -0.0076428(2) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0076762(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 229, rs = 30, polarized best variational -0.0224174(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.02250086(8) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 229, rs = 40, polarized best variational -0.0175008(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.01756580(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 229, rs = 50, polarized best variational -0.0143463(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144109(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 229, rs = 60, polarized best variational -0.0122010(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0122499(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 229, rs = 70, polarized best variational -0.0105951(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106443(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 229, rs = 80, polarized best variational -0.0093899(1) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0094294(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 232, rs = 30, N↑ = 145, N↓ = 87 best variational -0.0224340(6) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0225577(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 232, rs = 40, N↑ = 145, N↓ = 87 best variational -0.0174479(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175674(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 232, rs = 50, N↑ = 145, N↓ = 87 best variational -0.0143387(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144154(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 232, rs = 60, N↑ = 145, N↓ = 87 best variational -0.0121571(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0122349(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 232, rs = 70, N↑ = 145, N↓ = 87 best variational -0.0105717(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.01063722(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 232, rs = 80, N↑ = 145, N↓ = 87 best variational -0.0093482(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.00941375(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 244, rs = 100, N↑ = 183, N↓ = 61 best variational -0.0076400(1) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0076754(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 244, rs = 30, N↑ = 183, N↓ = 61 best variational -0.0225369(5) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0226077(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 244, rs = 40, N↑ = 183, N↓ = 61 best variational -0.0175366(6) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0176088(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 244, rs = 50, N↑ = 183, N↓ = 61 best variational -0.0143394(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144168(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 244, rs = 60, N↑ = 183, N↓ = 61 best variational -0.0122020(4) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0122585(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 244, rs = 70, N↑ = 183, N↓ = 61 best variational -0.0105734(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106399(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 244, rs = 80, N↑ = 183, N↓ = 61 best variational -0.0093813(3) VMC (SJB) Azadi & Drummond (2022)
best projected -0.0094298(1) FN-DMC (SJB) Azadi & Drummond (2022)
fcc cell, N = 274, rs = 30, unpolarized best variational -0.0224531(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0225566(3) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 274, rs = 40, unpolarized best variational -0.0174824(6) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0175674(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 274, rs = 50, unpolarized best variational -0.0143348(3) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0144121(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 274, rs = 60, unpolarized best variational -0.0121603(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0122328(1) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 274, rs = 70, unpolarized best variational -0.0105725(4) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0106352(2) FN-DMC (SJ) Azadi & Drummond (2022)
fcc cell, N = 274, rs = 80, unpolarized best variational -0.0093431(2) VMC (SJ) Azadi & Drummond (2022)
best projected -0.0094113(1) FN-DMC (SJ) Azadi & Drummond (2022)
rect-3x3x2 cell, N = 36, rs = 10, unpolarized best variational -0.0537396(1) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 100, unpolarized best variational -0.00769287(1) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 30, unpolarized best variational -0.02272554(2) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 5, unpolarized best variational -0.0756267(6) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 50, unpolarized best variational -0.01449795(2) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 80, unpolarized best variational -0.00945620(2) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 86.6, unpolarized best variational -0.00879026(2) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 86.7, unpolarized best variational -0.00878092(1) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 86.8, unpolarized best variational -0.00877159(1) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 86.9, unpolarized best variational -0.00876228(1) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 87, unpolarized best variational -0.008753017(8) VMC (MP-NQS) Liu et al. (2026)
rect-3x3x2 cell, N = 36, rs = 87.1, unpolarized best variational -0.008743822(8) VMC (MP-NQS) Liu et al. (2026)
sc cell, N = 7, rs = 1, polarized best variational 1.120358(3) VMC (WAP-net) Wilson et al. (2023)
best projected 1.120400(5) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 7, rs = 10, polarized best variational -0.0531436(2) VMC (WAP-net) Wilson et al. (2023)
best projected -0.0531380(5) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 7, rs = 100, polarized best variational -0.00774654(1) VMC (WAP-net) Wilson et al. (2023)
best projected -0.00774625(5) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 7, rs = 2, polarized best variational 0.110850(1) VMC (WAP-net) Wilson et al. (2023)
best projected 0.110879(2) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 7, rs = 20, polarized best variational -0.0322689(1) VMC (WAP-net) Wilson et al. (2023)
best projected -0.032266(2) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 7, rs = 5, polarized best variational -0.0664225(5) VMC (WAP-net) Wilson et al. (2023)
best projected -0.0664055(5) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 7, rs = 50, polarized best variational -0.01466089(1) VMC (WAP-net) Wilson et al. (2023)
best projected -0.0146604(1) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 14, rs = 0.1, unpolarized best projected 106.90015 ○ CCD Butler et al. (2024) butler-julie/HEG-SRE
best extrapolated 106.89994(1) CCSDT Spencer & Thom (2016)
best approximate 106.87643 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.2, unpolarized best extrapolated 25.4050004 ○ CCD Shepherd et al. (2014)
best approximate 25.3821433 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.3, unpolarized best extrapolated 10.6954209 ○ CCD Shepherd et al. (2014)
best approximate 10.6732066 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.4, unpolarized best extrapolated 5.6765448 ○ CCD Shepherd et al. (2014)
best approximate 5.6547591 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.5, unpolarized best variational 3.412684(4) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected 3.41253(4) ph-AFQMC (RHF) Lee et al. (2019) uses PAUXY
best extrapolated 3.41226(2) FCIQMC Shepherd et al. (2012)
best approximate 3.3916087 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.6, unpolarized best extrapolated 2.2154921 ○ CCD Shepherd et al. (2014)
best approximate 2.1945636 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.7, unpolarized best extrapolated 1.5130365 ○ CCD Shepherd et al. (2014)
best approximate 1.4923937 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.8, unpolarized best extrapolated 1.0698103 ○ CCD Shepherd et al. (2014)
best approximate 1.0493818 ○ dRPA Shepherd et al. (2014)
sc cell, N = 14, rs = 0.9, unpolarized best extrapolated 0.7746685 ○ CCD Shepherd et al. (2014)
best approximate 0.7534542 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 1, unpolarized best variational 0.568851(1) VMC (FermiNet) Liu et al. (2026)
best projected 0.56869(6) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
best extrapolated 0.56850(3) FCIQMC Shepherd et al. (2012)
best approximate 0.5464629 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 10, unpolarized best variational -0.0552126(6) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0552180(5) FN-DMC (iterative BF) Wilson et al. (2023)
best extrapolated -0.05289 ○ DCD Liao et al. (2021)
best approximate -0.0791573 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 100, unpolarized best variational -0.00773024(1) VMC (WAP-net) Wilson et al. (2023)
best projected -0.00773430(2) FN-DMC (iterative BF) Wilson et al. (2023)
best extrapolated -0.0064603 ○ CCD Shepherd et al. (2014)
best approximate -0.0104603 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 15, unpolarized best variational -0.0408619(1) VMC (FermiNet) Liu et al. (2026)
best approximate -0.0580244 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 2, unpolarized best variational -0.0084275(7) VMC (FermiNet) Cassella et al. (2023) uses FermiNet
best projected -0.00853(6) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
best extrapolated -0.00873(3) FCIQMC Shepherd et al. (2012)
best approximate -0.0478896 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 20, unpolarized best variational -0.0324553(2) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0324578(2) FN-DMC (iterative BF) Wilson et al. (2023)
best extrapolated -0.03035 ○ DCD Liao et al. (2021)
best approximate -0.0457024 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 3, unpolarized best projected -0.07352(4) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
best extrapolated -0.07432(2) CCSDTQ5 Neufeld & Thom (2017) uses HANDE-QMC
best approximate -0.1179136 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 30, unpolarized best extrapolated -0.0203291 ○ CCD Shepherd et al. (2014)
best approximate -0.0321148 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 4, unpolarized best extrapolated -0.0792519 ○ CCD Shepherd et al. (2014)
best approximate -0.1240376 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 40, unpolarized best extrapolated -0.0155875 ○ CCD Shepherd et al. (2014)
best approximate -0.0247303 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 5, unpolarized best variational -0.0798630(2) VMC (FermiNet) Liu et al. (2026)
best projected -0.079842(1) FN-DMC (iterative BF) Wilson et al. (2023)
best extrapolated -0.07997(7) FCIQMC Shepherd et al. (2012)
best approximate -0.1175392 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 50, unpolarized best variational -0.01462631(6) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0146287(1) FN-DMC (iterative BF) Wilson et al. (2023)
best extrapolated -0.01323 ○ DCD Liao et al. (2021)
best approximate -0.0201249 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 6, unpolarized best extrapolated -0.0706647 ○ CCD Shepherd et al. (2014)
best approximate -0.1085933 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 60, unpolarized best extrapolated -0.0106188 ○ CCD Shepherd et al. (2014)
best approximate -0.0169759 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 7, unpolarized best extrapolated -0.0651069 ○ CCD Shepherd et al. (2014)
best approximate -0.099964 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 70, unpolarized best extrapolated -0.0091195 ○ CCD Shepherd et al. (2014)
best approximate -0.0146909 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 8, unpolarized best extrapolated -0.0599259 ○ CCD Shepherd et al. (2014)
best approximate -0.0920688 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 80, unpolarized best extrapolated -0.0080403 ○ CCD Shepherd et al. (2014)
best approximate -0.0129689 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 9, unpolarized best extrapolated -0.0553862 ○ CCD Shepherd et al. (2014)
best approximate -0.0851719 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 14, rs = 90, unpolarized best extrapolated -0.0071484 ○ CCD Shepherd et al. (2014)
best approximate -0.0115769 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 19, rs = 1, polarized best variational 1.046242(3) VMC (WAP-net) Wilson et al. (2023)
best projected 1.0462250(5) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 19, rs = 10, polarized best variational -0.0528624(2) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0528652(3) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 19, rs = 100, polarized best variational -0.00771899(1) VMC (iterative BF) Wilson et al. (2023)
best projected -0.00772142(1) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 19, rs = 2, polarized best variational 0.096303(1) VMC (WAP-net) Wilson et al. (2023)
best projected 0.096302(2) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 19, rs = 20, polarized best variational -0.03201095(5) VMC (WAP-net) Wilson et al. (2023)
best projected -0.0320167(1) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 19, rs = 5, polarized best variational -0.0672510(2) VMC (WAP-net) Wilson et al. (2023)
best projected -0.0672540(5) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 19, rs = 50, polarized best variational -0.01456685(3) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.01456920(4) FN-DMC (iterative BF) Wilson et al. (2023)
sc cell, N = 27, rs = 1, polarized best variational 1.051771(4) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected 1.05200(3) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 27, rs = 10, polarized best variational -0.0526015(2) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.052540(6) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 27, rs = 2, polarized best variational 0.098460(2) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected 0.09866(2) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 27, rs = 30, polarized best variational -0.0228184(1) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0228080(8) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 27, rs = 5, polarized best variational -0.0665523(6) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.066429(4) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 27, rs = 50, polarized best variational -0.01457976(5) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0145752(6) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 27, rs = 70, polarized best variational -0.01074986(3) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.010749(2) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 27, rs = 90, polarized best variational -0.00853156(2) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0085314(5) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 38, rs = 0.5, unpolarized best projected 3.2080745 ○ CCD Butler et al. (2024) butler-julie/HEG-SRE
best extrapolated 3.20691(3) FCIQMC Shepherd et al. (2012)
sc cell, N = 38, rs = 1, unpolarized best extrapolated 0.52478(3) FCIQMC Shepherd et al. (2012)
sc cell, N = 38, rs = 2, unpolarized best extrapolated -0.01422(5) FCIQMC Shepherd et al. (2012)
sc cell, N = 54, rs = 0.5, unpolarized best variational 3.221226(2) VMC (DeepSolid) Li et al. (2022) bytedance/DeepSolid
best projected 3.22087(2) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
best extrapolated 3.2202(2) FCIQMC Shepherd et al. (2012)
best approximate 3.2119035 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 1, unpolarized best variational 0.52973(1) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected 0.52967(2) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
best extrapolated 0.52991(6) FCIQMC Shepherd et al. (2012)
best approximate 0.5147818 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 10, unpolarized best variational -0.054448(1) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.054443(2) FN-DMC (SJB) López Ríos et al. (2006) uses CASINO
best extrapolated -0.05157 ○ DCD Liao et al. (2021)
best approximate -0.0728389 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 100, unpolarized best variational -0.00769203(5) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.007674(3) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 54, rs = 15, unpolarized best extrapolated -0.0363669 ○ CCD Shepherd et al. (2014)
best approximate -0.0359224 ○ mCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 2, unpolarized best variational -0.014046(8) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.01429(3) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
best extrapolated -0.01286 ○ DCD Liao et al. (2021)
best approximate -0.0363623 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 20, unpolarized best variational -0.0320524(5) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.032047(2) FN-DMC (SJB) López Ríos et al. (2006) uses CASINO
best extrapolated -0.02925 ○ DCD Liao et al. (2021)
best approximate -0.0429947 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 3, unpolarized best approximate -0.0706229 ○ mCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 4, unpolarized best approximate -0.0774134 ○ mCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 5, unpolarized best variational -0.079090(2) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.079036(3) FN-DMC (SJB) López Ríos et al. (2006) uses CASINO
best extrapolated -0.07655 ○ DCD Liao et al. (2021)
best approximate -0.104002 ○ rxmCCD Shepherd et al. (2014)
sc cell, N = 54, rs = 50, unpolarized best variational -0.0145015(1) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.01387(2) FN-DMC (SJ) Pescia et al. (2024)
best extrapolated -0.01267 ○ DCD Liao et al. (2021)
best approximate -0.01281 ○ TC-DCD Liao et al. (2021)
sc cell, N = 54, rs = 7.5, unpolarized best approximate -0.0602626 ○ mCCD Shepherd et al. (2014)
sc cell, N = 66, rs = 1, unpolarized best variational 0.5748(3) VMC (SJ) Kwon et al. (1998)
best projected 0.57290(3) FN-DMC Fantoni (2013)
sc cell, N = 66, rs = 10, unpolarized best variational -0.05318(1) VMC (SJ) Kwon et al. (1998)
best projected -0.053728(3) FN-DMC Fantoni (2013)
sc cell, N = 66, rs = 2, unpolarized best projected -0.00208(4) FN-DMC Fantoni (2013)
sc cell, N = 66, rs = 20, unpolarized best variational -0.031515(5) VMC (SJ) Kwon et al. (1998)
sc cell, N = 66, rs = 5, unpolarized best variational -0.07583(2) VMC (SJ) Kwon et al. (1998)
best projected -0.076676(2) FN-DMC Fantoni (2013)
sc cell, N = 114, rs = 0.5, unpolarized best projected 3.48453(8) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
sc cell, N = 114, rs = 1, unpolarized best variational 0.6039(3) VMC (SJ) Kwon et al. (1998)
best projected 0.59877(6) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
sc cell, N = 114, rs = 10, unpolarized best variational -0.05276(1) VMC (SJ) Kwon et al. (1998)
sc cell, N = 114, rs = 2, unpolarized best projected 0.00487(6) ph-AFQMC (RHF) Lee et al. (2019) uses QMCPACK
sc cell, N = 114, rs = 20, unpolarized best variational -0.031390(5) VMC (SJ) Kwon et al. (1998)
sc cell, N = 114, rs = 5, unpolarized best variational -0.07433(1) VMC (SJ) Kwon et al. (1998)
sc cell, N = 128, rs = 110, unpolarized best variational -0.0071121(2) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.007009518(1) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 128, rs = 200, unpolarized best variational -0.0040615(1) VMC (MP-NQS) Pescia et al. (2024) uses NetKet 3
best projected -0.0039923(7) FN-DMC (SJ) Pescia et al. (2024)
sc cell, N = 162, rs = 1, unpolarized best variational 0.5581(2) VMC (SJ) Kwon et al. (1998)
sc cell, N = 162, rs = 10, unpolarized best variational -0.053210(5) VMC (SJ) Kwon et al. (1998)
sc cell, N = 162, rs = 20, unpolarized best variational -0.031350(5) VMC (SJ) Kwon et al. (1998)
sc cell, N = 162, rs = 5, unpolarized best variational -0.07619(1) VMC (SJ) Kwon et al. (1998)
sc cell, N = 246, rs = 1, unpolarized best variational 0.5969(2) VMC (SJ) Kwon et al. (1998)
sc cell, N = 246, rs = 10, unpolarized best variational -0.052740(5) VMC (SJ) Kwon et al. (1998)
sc cell, N = 246, rs = 20, unpolarized best variational -0.031375(5) VMC (SJ) Kwon et al. (1998)
sc cell, N = 246, rs = 5, unpolarized best variational -0.07443(2) VMC (SJ) Kwon et al. (1998)
Electron gas, 2D: 65 instances, energies as E/N (Ha)
instance value energy method code
square cell, N = 21, rs = 10, polarized best variational -0.08492(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 21, rs = 20, polarized best variational -0.04634(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 21, rs = 30, polarized best variational -0.031965(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 21, rs = 40, polarized best variational -0.024434(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 21, rs = 5, polarized best variational -0.1451(1) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 21, rs = 75, polarized best variational -0.013457(1) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 26, rs = 1, unpolarized best variational -0.1850(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 26, rs = 10, unpolarized best variational -0.08433(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 26, rs = 20, unpolarized best variational -0.04587(1) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 26, rs = 30, unpolarized best variational -0.03166(1) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 26, rs = 5, unpolarized best variational -0.14685(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 26, rs = 50, unpolarized best variational -0.019659(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 37, rs = 10, polarized best variational -0.08440(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 37, rs = 20, polarized best variational -0.04614(1) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 37, rs = 30, polarized best variational -0.0318870(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 37, rs = 40, polarized best variational -0.024379(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 37, rs = 5, polarized best variational -0.14373(4) VMC (NCT) Xie et al. (2023) fermiflow/CoulombGas
square cell, N = 37, rs = 75, polarized best variational -0.0134380(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 42, rs = 1, unpolarized best variational -0.2225(3) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 42, rs = 10, unpolarized best variational -0.08450(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 42, rs = 20, unpolarized best variational -0.04588(1) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 42, rs = 30, unpolarized best variational -0.031675(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 42, rs = 5, unpolarized best variational -0.14800(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 42, rs = 50, unpolarized best variational -0.019654(3) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 57, rs = 10, polarized best variational -0.08390(5) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.08427(3) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 57, rs = 20, polarized best variational -0.04607(3) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.04618(1) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 57, rs = 30, polarized best variational -0.031825(5) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.031913(4) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 57, rs = 40, polarized best variational -0.024360(5) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.024420(1) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 57, rs = 5, polarized best variational -0.14225(5) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.14291(5) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 57, rs = 75, polarized best variational -0.0134275(5) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.013473(2) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 58, rs = 1, unpolarized best variational -0.1953(1) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.2046(3) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 58, rs = 10, unpolarized best variational -0.08426(2) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.08552(4) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 58, rs = 20, unpolarized best variational -0.04582(2) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.04636(1) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 58, rs = 30, unpolarized best variational -0.031655(3) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.031967(3) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 58, rs = 5, unpolarized best variational -0.1470(1) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.14990(5) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 58, rs = 50, unpolarized best variational -0.019651(3) VMC (SJ) Tanatar & Ceperley (1989)
best projected -0.019763(3) FN-GFMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 69, rs = 10, polarized best variational -0.08412(3) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 69, rs = 20, polarized best variational -0.046085(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 69, rs = 30, polarized best variational -0.031852(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 69, rs = 40, polarized best variational -0.024375(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 69, rs = 5, polarized best variational -0.14310(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 69, rs = 75, polarized best variational -0.0134305(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 74, rs = 1, unpolarized best variational -0.2078(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 74, rs = 10, unpolarized best variational -0.08429(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 74, rs = 20, unpolarized best variational -0.045845(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 74, rs = 30, unpolarized best variational -0.031662(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 74, rs = 5, unpolarized best variational -0.14735(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 74, rs = 50, unpolarized best variational -0.019651(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 90, rs = 30, unpolarized best variational -0.0317373(2) VMC (SJ) Azadi et al. (2024) uses CASINO
best projected -0.031919(1) FN-DMC Azadi et al. (2024) uses CASINO
square cell, N = 113, rs = 10, polarized best variational -0.08396(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 113, rs = 20, polarized best variational -0.046030(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 113, rs = 30, polarized best variational -0.031821(3) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 113, rs = 40, polarized best variational -0.024356(2) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 113, rs = 5, polarized best variational -0.14215(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 113, rs = 75, polarized best variational -0.0134245(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 114, rs = 1, unpolarized best variational -0.1983(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 114, rs = 10, unpolarized best variational -0.08423(1) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 114, rs = 20, unpolarized best variational -0.045825(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 114, rs = 30, unpolarized best variational -0.031647(4) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 114, rs = 5, unpolarized best variational -0.14685(5) VMC (SJ) Tanatar & Ceperley (1989)
square cell, N = 114, rs = 50, unpolarized best variational -0.019648(2) VMC (SJ) Tanatar & Ceperley (1989)
triangular cell, N = 16, rs = 30, polarized best variational -0.031990687(3) VMC (Fermi Sets) Li et al. (2026)
best projected -0.03199636(7) FP-DMC (Fermi Sets) Li et al. (2026)
triangular cell, N = 91, rs = 30, polarized best variational -0.03193763(3) VMC (self-attention) Gaggioli et al. (2026)
best projected -0.0319370(1) FN-DMC (SJB) Gaggioli et al. (2026)
triangular cell, N = 91, rs = 40, polarized best variational -0.02443814(2) VMC (self-attention) Gaggioli et al. (2026)
best projected -0.0244377(2) FN-DMC (SJB) Gaggioli et al. (2026)
triangular cell, N = 169, rs = 30, polarized best variational -0.03192077(3) VMC (self-attention) Gaggioli et al. (2026)
best projected -0.0319197(1) FN-DMC (SJB) Gaggioli et al. (2026)
Hydrogen chain: 228 instances, energies as E/N (Ha)
instance value energy method code
H4 chain, open, R = 1.51178, STO-3G exact -0.5418901 FCI QMBL check, checks/hchain-fci/ QMBL code
best variational -0.5418875 ○ (+2.6e-6) VQE Li et al. (2023) tencent-quantum-lab/TenCirChem
H4 chain, open, R = 1.8, STO-6G exact -0.547595 FCI Li et al. (2023)
best variational -0.547595 ○ (+<1e-6) VMC (RBM) Li et al. (2023)
H4 chain, open, R = 3.6, STO-6G exact -0.481645 FCI Li et al. (2023)
best variational -0.481645 ○ (+<1e-6) VMC (RBM) Li et al. (2023)
H6 chain, open, R = 1.51178, STO-3G exact -0.5340686 FCI QMBL check, checks/hchain-fci/ QMBL code
best variational -0.5340233 ○ (+4.5e-5) VQE Li et al. (2023) tencent-quantum-lab/TenCirChem
H6 chain, open, R = 1.8, STO-6G exact -0.5444567 FCI Li et al. (2023)
best variational -0.5444567 ○ (+<1e-7) VMC (RBM) Li et al. (2023)
best approximate -0.5444567 ○ (+<1e-7) CCSD(T) Li et al. (2023)
H6 chain, open, R = 2, STO-3G exact -0.5362833 ED Kowalski & Bauman (2023)
best variational -0.5362167 ○ (+6.7e-5) QFlow Kowalski & Bauman (2023)
best projected -0.5363333 ○ (−5.0e-5) CCSDT Kowalski & Bauman (2023)
H6 chain, open, R = 2.83459, STO-6G exact -0.5033663 FCI Stair et al. (2020)
H6 chain, open, R = 3, cc-pVDZ exact -0.5265167 ED Kowalski & Bauman (2023)
best projected -0.5265167 ○ (+<1e-7) CCSDTQ Kowalski & Bauman (2023)
best approximate -0.5264833 ○ (+3.3e-5) DUCC-QFlow Kowalski & Bauman (2023)
H6 chain, open, R = 3, STO-3G exact -0.4929333 ED Kowalski & Bauman (2023)
best variational -0.4920167 ○ (+9.2e-4) QFlow Kowalski & Bauman (2023)
best projected -0.4929 ○ (+3.3e-5) CCSDTQ Kowalski & Bauman (2023)
H6 chain, open, R = 3.6, STO-6G exact -0.4817533 FCI Li et al. (2023)
best variational -0.4817517 ○ (+1.7e-6) VMC (RBM) Li et al. (2023)
H8 chain, open, R = 1.51178, STO-3G exact -0.5304239 FCI QMBL check, checks/hchain-fci/ QMBL code
best variational -0.530315 ○ (+1.1e-4) VQE Li et al. (2023) tencent-quantum-lab/TenCirChem
H8 chain, open, R = 1.8, STO-6G exact -0.543135 FCI Li et al. (2023)
best variational -0.5431337 ○ (+1.3e-6) VMC (RBM) Li et al. (2023)
best approximate -0.543125 ○ (+1.0e-5) CCSD(T) Li et al. (2023)
H8 chain, open, R = 2, STO-3G exact -0.53575 ED Kowalski & Bauman (2023)
best variational -0.5355875 ○ (+1.6e-4) QFlow Kowalski & Bauman (2023)
best projected -0.53575 ○ (+<1e-5) CCSDTQ Kowalski & Bauman (2023)
H8 chain, open, R = 2.83459, STO-6G exact -0.503519 FCI Stair et al. (2020)
H8 chain, open, R = 3, STO-3G exact -0.4930875 ED Kowalski & Bauman (2023)
best variational -0.491525 ○ (+1.6e-3) QFlow Kowalski & Bauman (2023)
best projected -0.4929875 ○ (+1.0e-4) CCSDTQ Kowalski & Bauman (2023)
H8 chain, open, R = 3.6, STO-6G exact -0.4818225 FCI Li et al. (2023)
best variational -0.4818188 ○ (+3.7e-6) VMC (RBM) Li et al. (2023)
H10 chain, open, R = 1, aug-cc-pVQZ best variational -0.41566 ○ HF Motta et al. (2020)
best approximate -0.43918 ○ MP2 Motta et al. (2020)
H10 chain, open, R = 1, aug-cc-pVTZ best variational -0.41495 ○ HF Motta et al. (2020)
best projected -0.44012 ○ CCSD Motta et al. (2020)
best approximate -0.43752 ○ MP2 Motta et al. (2020)
H10 chain, open, R = 1, cc-pV5Z best variational -0.4155 ○ HF Motta et al. (2020)
best projected -0.44236(8) ph-AFQMC Motta et al. (2017)
best approximate -0.43927 ○ MP2 Motta et al. (2020)
H10 chain, open, R = 1, cc-pVDZ best variational -0.42186 ○ DMRG Motta et al. (2017)
best projected -0.4220847 ○ DMET Motta et al. (2017)
best approximate -0.4217751 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1, cc-pVQZ best variational -0.41505 ○ HF Motta et al. (2020)
best projected -0.44160(8) ph-AFQMC Motta et al. (2017)
best approximate -0.4413939 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1, cc-pVTZ best variational -0.4395 ○ DMRG Motta et al. (2017)
best projected -0.43969(6) ph-AFQMC Motta et al. (2017)
best approximate -0.4394551 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1, basis-free best variational -0.441499(9) VMC (JAGP) Motta et al. (2017)
best projected -0.442430(7) LR-DMC (AGP) Motta et al. (2017)
best extrapolated -0.4432(3) MRCI+Q Motta et al. (2017)
best approximate -0.4427(2) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1, STO-6G exact -0.3824389 FCI Motta et al. (2017)
best variational -0.3824389 ○ (−<1e-7) MRCI Motta et al. (2017)
best projected -0.38248(3) (−4.1e-5) ph-AFQMC Motta et al. (2017)
best approximate -0.382432 ○ (+6.9e-6) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.2, cc-pV5Z best variational -0.4884091 ○ HF Motta et al. (2017)
best projected -0.51451(6) ph-AFQMC Motta et al. (2017)
H10 chain, open, R = 1.2, cc-pVDZ best variational -0.50271 ○ DMRG Motta et al. (2017)
best projected -0.5029843 ○ DMET Motta et al. (2017)
best approximate -0.506634 ○ GW Motta et al. (2017)
H10 chain, open, R = 1.2, cc-pVQZ best variational -0.4882713 ○ HF Motta et al. (2017)
best projected -0.51419(8) ph-AFQMC Motta et al. (2017)
best approximate -0.5140214 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.2, cc-pVTZ best variational -0.51302 ○ DMRG Motta et al. (2017)
best projected -0.51315(9) ph-AFQMC Motta et al. (2017)
best approximate -0.5129509 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.2, basis-free best variational -0.513646(9) VMC (JAGP) Motta et al. (2017)
best projected -0.514432(6) LR-DMC (AGP) Motta et al. (2017)
best extrapolated -0.5153(2) MRCI+Q Motta et al. (2017)
best approximate -0.5149(2) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.2, STO-6G exact -0.4766378 FCI Motta et al. (2017)
best variational -0.4766378 ○ (−<1e-7) DMRG Motta et al. (2017)
best projected -0.476638 ○ (−2.3e-7) CCSDT Low et al. (2019)
best approximate -0.4766261 ○ (+1.2e-5) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.4, cc-pV5Z best variational -0.5228716 ○ HF Motta et al. (2017)
best projected -0.54871(9) ph-AFQMC Motta et al. (2017)
H10 chain, open, R = 1.4, cc-pVDZ best variational -0.54087 ○ DMRG Motta et al. (2017)
best projected -0.5411661 ○ DMET Motta et al. (2017)
best approximate -0.54465 ○ GW Motta et al. (2017)
H10 chain, open, R = 1.4, cc-pVQZ best variational -0.547832 ○ MRCI Motta et al. (2017)
best projected -0.54855(5) ph-AFQMC Motta et al. (2017)
best approximate -0.5483736 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.4, cc-pVTZ best variational -0.54769 ○ DMRG Motta et al. (2017)
best projected -0.5477564 ○ MRCI+Q Motta et al. (2017)
best approximate -0.547569 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.4, basis-free best variational -0.548046(7) VMC (JAGP) Motta et al. (2017)
best projected -0.548748(7) LR-DMC (LDA determinant) Motta et al. (2017)
best extrapolated -0.5493(2) MRCI+Q Motta et al. (2017)
best approximate -0.5491(1) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.4, STO-6G exact -0.5205094 FCI Motta et al. (2017)
best variational -0.5205094 ○ (−<1e-7) MRCI Motta et al. (2017)
best projected -0.52051(5) (−5.9e-7) ph-AFQMC Motta et al. (2017)
best approximate -0.520492 ○ (+1.7e-5) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.41729, STO-6G exact -0.522856 FCI Stair & Evangelista (2020)
H10 chain, open, R = 1.51178, STO-3G exact -0.5283552 FCI QMBL check, checks/hchain-fci/ QMBL code
best variational -0.528221 ○ (+1.3e-4) VQE Li et al. (2023) tencent-quantum-lab/TenCirChem
H10 chain, open, R = 1.6, cc-pV5Z best variational -0.5368359 ○ HF Motta et al. (2017)
best projected -0.5629322 ○ MRCI+Q Motta et al. (2017)
H10 chain, open, R = 1.6, cc-pVDZ best variational -0.55702 ○ DMRG Motta et al. (2017)
best projected -0.5573602 ○ DMET Motta et al. (2017)
best approximate -0.56045 ○ GW Motta et al. (2017)
H10 chain, open, R = 1.6, cc-pVQZ best variational -0.5620252 ○ MRCI Motta et al. (2017)
best projected -0.5627104 ○ MRCI+Q Motta et al. (2017)
best approximate -0.562514 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.6, cc-pVTZ best variational -0.56191 ○ DMRG Motta et al. (2017)
best projected -0.5620(1) ph-AFQMC Motta et al. (2017)
best approximate -0.5617783 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.6, basis-free best variational -0.562237(5) VMC (JAGP) Motta et al. (2017)
best projected -0.562900(7) LR-DMC (LDA determinant) Motta et al. (2017)
best extrapolated -0.56325(8) MRCI+Q Motta et al. (2017)
best approximate -0.56311(9) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.6, STO-6G exact -0.5384361 FCI Motta et al. (2017)
best variational -0.5384361 ○ (+<1e-7) MRCI Motta et al. (2017)
best projected -0.5384361 ○ (+<1e-7) MRCI+Q Motta et al. (2017)
best approximate -0.5384141 ○ (+2.2e-5) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.8, cc-pV5Z best variational -0.5401556 ○ HF Motta et al. (2017)
best projected -0.566277 ○ MRCI+Q Motta et al. (2017)
H10 chain, open, R = 1.8, cc-pVDZ best variational -0.56141 ○ DMRG Motta et al. (2017)
best projected -0.5618118 ○ DMET Motta et al. (2017)
best approximate -0.564291 ○ GW Motta et al. (2017)
H10 chain, open, R = 1.8, cc-pVQZ best variational -0.5654171 ○ MRCI Motta et al. (2017)
best projected -0.5660681 ○ MRCI+Q Motta et al. (2017)
best approximate -0.5658519 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.8, cc-pVTZ best variational -0.56523 ○ DMRG Motta et al. (2017)
best projected -0.5653303 ○ MRCI+Q Motta et al. (2017)
best approximate -0.5651061 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.8, basis-free best variational -0.565634(5) VMC (JAGP) Motta et al. (2017)
best projected -0.566255(7) LR-DMC (LDA determinant) Motta et al. (2017)
best extrapolated -0.5667(1) SBDMRG Motta et al. (2017)
best approximate -0.56638(4) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 1.8, STO-6G exact -0.5424385 FCI Motta et al. (2017)
best variational -0.5424385 ○ (−<1e-7) MRCI Motta et al. (2017)
best projected -0.542439 ○ (−4.6e-7) CCSDTQ Low et al. (2019)
best approximate -0.542419 ○ (+2.0e-5) CCSD(T) Li et al. (2023)
H10 chain, open, R = 1.88973, STO-6G exact -0.5415393 FCI Stair & Evangelista (2020)
H10 chain, open, R = 2, cc-pV5Z best variational -0.538217 ○ HF Motta et al. (2017)
best projected -0.5638526 ○ MRCI+Q Motta et al. (2017)
H10 chain, open, R = 2, cc-pVDZ best variational -0.55949 ○ DMRG Motta et al. (2017)
best projected -0.5599357 ○ DMET Motta et al. (2017)
best approximate -0.561647 ○ GW Motta et al. (2017)
H10 chain, open, R = 2, cc-pVQZ best variational -0.563033 ○ MRCI Motta et al. (2017)
best projected -0.5636456 ○ MRCI+Q Motta et al. (2017)
best approximate -0.5634155 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2, cc-pVTZ best variational -0.56282 ○ DMRG Motta et al. (2017)
best projected -0.5628926 ○ MRCI+Q Motta et al. (2017)
best approximate -0.562658 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2, basis-free best variational -0.563249(4) VMC (JAGP) Motta et al. (2017)
best projected -0.563852(7) LR-DMC (LDA determinant) Motta et al. (2017)
best extrapolated -0.5643(1) SBDMRG Motta et al. (2017)
best approximate -0.56391(1) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2, STO-6G exact -0.5389626 FCI Motta et al. (2017)
best variational -0.5389626 ○ (−<1e-7) DMRG Motta et al. (2017)
best projected -0.538963 ○ (−4.1e-7) CCSDTQ Low et al. (2019)
best approximate -0.5380497 ○ (+9.1e-4) UCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.4, cc-pV5Z best variational -0.5281156 ○ HF Motta et al. (2017)
best projected -0.5516514 ○ MRCI+Q Motta et al. (2017)
H10 chain, open, R = 2.4, cc-pVDZ best variational -0.54761 ○ DMRG Motta et al. (2017)
best projected -0.5480704 ○ DMET Motta et al. (2017)
best approximate -0.547728 ○ GW Motta et al. (2017)
H10 chain, open, R = 2.4, cc-pVQZ best variational -0.5509118 ○ MRCI Motta et al. (2017)
best projected -0.5514268 ○ MRCI+Q Motta et al. (2017)
best approximate -0.5512171 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.4, cc-pVTZ best variational -0.55059 ○ DMRG Motta et al. (2017)
best projected -0.5506631 ○ MRCI+Q Motta et al. (2017)
best approximate -0.550459 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.4, basis-free best variational -0.551106(4) VMC (JAGP) Motta et al. (2017)
best projected -0.551699(8) LR-DMC (LDA determinant) Motta et al. (2017)
best extrapolated -0.5520(1) SBDMRG Motta et al. (2017)
best approximate -0.55167(3) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.4, STO-6G exact -0.5227936 FCI Motta et al. (2017)
best variational -0.5227936 ○ (+<1e-7) MRCI Motta et al. (2017)
best projected -0.522794 ○ (−3.5e-7) CCSDTQ Low et al. (2019)
best approximate -0.5207534 ○ (+2.0e-3) UCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.8, cc-pV5Z best variational -0.5174129 ○ HF Motta et al. (2017)
best projected -0.53749(7) ph-AFQMC Motta et al. (2017)
H10 chain, open, R = 2.8, cc-pVDZ best variational -0.53344 ○ DMRG Motta et al. (2017)
best projected -0.5347972 ○ SEET Motta et al. (2017)
best approximate -0.5336142 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.8, cc-pVQZ best variational -0.5367131 ○ MRCI Motta et al. (2017)
best projected -0.5370991 ○ MRCI+Q Motta et al. (2017)
best approximate -0.5370925 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.8, cc-pVTZ best variational -0.53626 ○ DMRG Motta et al. (2017)
best projected -0.53633(5) ph-AFQMC Motta et al. (2017)
best approximate -0.5363253 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.8, basis-free best variational -0.536832(3) VMC (JAGP) Motta et al. (2017)
best projected -0.537424(9) LR-DMC (LDA determinant) Motta et al. (2017)
best extrapolated -0.5377(1) SBDMRG Motta et al. (2017)
best approximate -0.53749(6) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.8, STO-6G exact -0.5050245 FCI Motta et al. (2017)
best variational -0.5050245 ○ (−<1e-7) MRCI Motta et al. (2017)
best projected -0.50507(5) (−4.6e-5) ph-AFQMC Motta et al. (2017)
best approximate -0.5029597 ○ (+2.1e-3) UCCSD(T) Motta et al. (2017)
H10 chain, open, R = 2.83459, STO-6G exact -0.5036293 FCI Stair & Evangelista (2020)
H10 chain, open, R = 3.2, cc-pV5Z best variational -0.5096605 ○ HF Motta et al. (2017)
best projected -0.52525(5) ph-AFQMC Motta et al. (2017)
H10 chain, open, R = 3.2, cc-pVDZ best variational -0.52125 ○ DMRG Motta et al. (2017)
best projected -0.5234726 ○ SEET Motta et al. (2017)
best approximate -0.5228438 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.2, cc-pVQZ best variational -0.5243413 ○ MRCI Motta et al. (2017)
best projected -0.52488(5) ph-AFQMC Motta et al. (2017)
best approximate -0.5254869 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.2, cc-pVTZ best variational -0.52382 ○ DMRG Motta et al. (2017)
best projected -0.52417(5) ph-AFQMC Motta et al. (2017)
best approximate -0.5248344 ○ RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.2, basis-free best variational -0.524373(4) VMC (JAGP) Motta et al. (2017)
best projected -0.524987(7) LR-DMC (AGP) Motta et al. (2017)
best extrapolated -0.52512(6) DMET Motta et al. (2017)
best approximate -0.5257(1) RCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.2, STO-6G exact -0.4910383 FCI Motta et al. (2017)
best variational -0.4910383 ○ (−<1e-7) MRCI Motta et al. (2017)
best projected -0.4910383 ○ (−<1e-7) MRCI+Q Motta et al. (2017)
best approximate -0.4895218 ○ (+1.5e-3) UCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.6, cc-pV5Z best variational -0.5050291 ○ HF Motta et al. (2017)
best projected -0.51584(8) ph-AFQMC Motta et al. (2017)
H10 chain, open, R = 3.6, cc-pVDZ best variational -0.51238 ○ DMRG Motta et al. (2017)
best projected -0.51287(3) ph-AFQMC Motta et al. (2017)
best approximate -0.5119131 ○ PC-NEVPT2 Motta et al. (2017)
H10 chain, open, R = 3.6, cc-pVQZ best variational -0.5150225 ○ MRCI Motta et al. (2017)
best projected -0.51580(5) ph-AFQMC Motta et al. (2017)
best approximate -0.514026 ○ UCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.6, cc-pVTZ best variational -0.51448 ○ DMRG Motta et al. (2017)
best projected -0.51507(3) ph-AFQMC Motta et al. (2017)
best approximate -0.513382 ○ PC-NEVPT2 Motta et al. (2017)
H10 chain, open, R = 3.6, basis-free best variational -0.514968(3) VMC (JAGP) Motta et al. (2017)
best projected -0.51558(1) LR-DMC (LDA determinant) Motta et al. (2017)
best extrapolated -0.51612(9) DMET Motta et al. (2017)
best approximate -0.5143(1) UCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.6, STO-6G exact -0.4818701 FCI Motta et al. (2017)
best variational -0.4818701 ○ (+<1e-7) MRCI Motta et al. (2017)
best projected -0.4818701 ○ (+<1e-7) MRCI+Q Motta et al. (2017)
best approximate -0.4809595 ○ (+9.1e-4) UCCSD(T) Motta et al. (2017)
H10 chain, open, R = 3.77945, STO-6G exact -0.4790989 FCI Stair & Evangelista (2020)
H12 chain, open, R = 1.51178, STO-3G exact -0.5270349 FCI QMBL check, checks/hchain-fci/ QMBL code
best variational -0.5268575 ○ (+1.8e-4) VQE Li et al. (2023) tencent-quantum-lab/TenCirChem
H12 chain, open, R = 1.8, STO-6G exact -0.5420192 FCI Li et al. (2023)
best variational -0.5420125 ○ (+6.7e-6) VMC (RBM) Li et al. (2023)
best approximate -0.5419892 ○ (+3.0e-5) CCSD(T) Li et al. (2023)
H12 chain, open, R = 1.88973, STO-3G exact -0.5377347 ED Huang et al. (2026)
H12 chain, open, R = 3.6, STO-6G exact -0.4819042 FCI Li et al. (2023)
best variational -0.4819025 ○ (+1.7e-6) VMC (RBM) Li et al. (2023)
H14 chain, open, R = 1.51178, STO-3G exact -0.5261238 FCI QMBL check, checks/hchain-fci/ QMBL code
best variational -0.525915 ○ (+2.1e-4) VQE Li et al. (2023) tencent-quantum-lab/TenCirChem
H16 chain, open, R = 1.51178, STO-3G exact -0.5254592 FCI QMBL check, checks/hchain-fci/ QMBL code
best variational -0.5252269 ○ (+2.3e-4) VQE Li et al. (2023) tencent-quantum-lab/TenCirChem
H20 chain, open, R = 3.6, STO-6G best projected -0.481978(1) FCIQMC Guther et al. (2020) ghb24/NECI_STABLE
H22 chain, open, R = 1, STO-6G best projected -0.357541(9) ph-AFQMC Motta et al. (2017)
H22 chain, open, R = 1.4, STO-6G best projected -0.51444(1) ph-AFQMC Motta et al. (2017)
H22 chain, open, R = 1.8, STO-6G best projected -0.54115(2) ph-AFQMC Motta et al. (2017)
H22 chain, open, R = 2.8, STO-6G best projected -0.50541(2) ph-AFQMC Motta et al. (2017)
H30 chain, open, R = 1, cc-pV5Z best variational -0.3969058 ○ HF Motta et al. (2017)
H30 chain, open, R = 1, cc-pVDZ best variational -0.3937633 ○ DMRG Motta et al. (2017)
best projected -0.39379(3) ph-AFQMC Motta et al. (2017)
best approximate -0.3936663 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1, cc-pVQZ best variational -0.3948131 ○ HF Motta et al. (2017)
best projected -0.42184(7) ph-AFQMC Motta et al. (2017)
best approximate -0.421883 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1, cc-pVTZ best variational -0.3898388 ○ HF Motta et al. (2017)
best projected -0.41760(3) ph-AFQMC Motta et al. (2017)
best approximate -0.41743 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1, basis-free best variational -0.42157(2) VMC (SJ) Motta et al. (2017)
best projected -0.42510(3) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 1, STO-6G best variational -0.3518877 ○ DMRG Motta et al. (2017)
best projected -0.3528238 ○ DMET Motta et al. (2017)
best approximate -0.35206 ○ GW Motta et al. (2017)
H30 chain, open, R = 1.2, cc-pV5Z best variational -0.4739482 ○ HF Motta et al. (2017)
H30 chain, open, R = 1.2, cc-pVDZ best variational -0.4891083 ○ DMRG Motta et al. (2017)
best projected -0.48927(3) ph-AFQMC Motta et al. (2017)
best approximate -0.489002 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.2, cc-pVQZ best variational -0.4736828 ○ HF Motta et al. (2017)
best projected -0.50143(5) ph-AFQMC Motta et al. (2017)
best approximate -0.5011587 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.2, cc-pVTZ best variational -0.4731441 ○ HF Motta et al. (2017)
best projected -0.50030(3) ph-AFQMC Motta et al. (2017)
best approximate -0.4999623 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.2, basis-free best variational -0.50020(1) VMC (SJ) Motta et al. (2017)
best projected -0.50177(2) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 1.2, STO-6G best variational -0.461805 ○ DMRG Motta et al. (2017)
best projected -0.4627503 ○ DMET Motta et al. (2017)
best approximate -0.4617621 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.4, cc-pV5Z best variational -0.5155844 ○ HF Motta et al. (2017)
H30 chain, open, R = 1.4, cc-pVDZ best variational -0.5344613 ○ DMRG Motta et al. (2017)
best projected -0.5354635 ○ DMET Motta et al. (2017)
best approximate -0.5343077 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.4, cc-pVQZ best variational -0.5154895 ○ HF Motta et al. (2017)
best projected -0.54253(5) ph-AFQMC Motta et al. (2017)
best approximate -0.542323 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.4, cc-pVTZ best variational -0.5152041 ○ HF Motta et al. (2017)
best projected -0.54186(3) ph-AFQMC Motta et al. (2017)
best approximate -0.5414947 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.4, basis-free best variational -0.54142(1) VMC (SJ) Motta et al. (2017)
best projected -0.54276(1) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 1.4, STO-6G best variational -0.5132063 ○ DMRG Motta et al. (2017)
best projected -0.5140977 ○ DMET Motta et al. (2017)
best approximate -0.5131409 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.6, cc-pV5Z best variational -0.5337486 ○ HF Motta et al. (2017)
H30 chain, open, R = 1.6, cc-pVDZ best variational -0.5542583 ○ DMRG Motta et al. (2017)
best projected -0.55440(3) ph-AFQMC Motta et al. (2017)
best approximate -0.5540527 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.6, cc-pVQZ best variational -0.5336765 ○ HF Motta et al. (2017)
best projected -0.55999(7) ph-AFQMC Motta et al. (2017)
best approximate -0.5599073 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.6, cc-pVTZ best variational -0.5334553 ○ HF Motta et al. (2017)
best projected -0.55942(3) ph-AFQMC Motta et al. (2017)
best approximate -0.559162 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.6, basis-free best variational -0.559065(9) VMC (SJ) Motta et al. (2017)
best projected -0.56038(1) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 1.6, STO-6G best variational -0.534978 ○ DMRG Motta et al. (2017)
best projected -0.5357627 ○ DMET Motta et al. (2017)
best approximate -0.534889 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.8, cc-pV5Z best variational -0.5394784 ○ HF Motta et al. (2017)
H30 chain, open, R = 1.8, cc-pVDZ best variational -0.560521 ○ DMRG Motta et al. (2017)
best projected -0.5616303 ○ DMET Motta et al. (2017)
best approximate -0.560279 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.8, cc-pVQZ best variational -0.5394138 ○ HF Motta et al. (2017)
best projected -0.56530(5) ph-AFQMC Motta et al. (2017)
best approximate -0.564994 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.8, cc-pVTZ best variational -0.5392194 ○ HF Motta et al. (2017)
best projected -0.56451(3) ph-AFQMC Motta et al. (2017)
best approximate -0.564239 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 1.8, basis-free best variational -0.564180(9) VMC (SJ) Motta et al. (2017)
best projected -0.56550(1) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 1.8, STO-6G best variational -0.5409897 ○ DMRG Motta et al. (2017)
best projected -0.5416268 ○ DMET Motta et al. (2017)
best approximate -0.5408894 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2, cc-pV5Z best variational -0.5386818 ○ HF Motta et al. (2017)
H30 chain, open, R = 2, cc-pVDZ best variational -0.5595467 ○ DMRG Motta et al. (2017)
best projected -0.55961(2) ph-AFQMC Motta et al. (2017)
best approximate -0.55928 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2, cc-pVQZ best variational -0.5386235 ○ HF Motta et al. (2017)
best projected -0.56379(4) ph-AFQMC Motta et al. (2017)
best approximate -0.5634263 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2, cc-pVTZ best variational -0.5384493 ○ HF Motta et al. (2017)
best projected -0.56295(3) ph-AFQMC Motta et al. (2017)
best approximate -0.5626683 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2, basis-free best variational -0.562636(9) VMC (SJ) Motta et al. (2017)
best projected -0.56403(1) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 2, STO-6G best variational -0.5385523 ○ DMRG Motta et al. (2017)
best projected -0.5390239 ○ DMET Motta et al. (2017)
best approximate -0.5384874 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2.4, cc-pV5Z best variational -0.5292216 ○ HF Motta et al. (2017)
H30 chain, open, R = 2.4, cc-pVDZ best variational -0.5482932 ○ DMRG Motta et al. (2017)
best projected -0.5493137 ○ DMET Motta et al. (2017)
best approximate -0.5480643 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2.4, cc-pVQZ best variational -0.5291749 ○ HF Motta et al. (2017)
best projected -0.55215(4) ph-AFQMC Motta et al. (2017)
best approximate -0.5517193 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2.4, cc-pVTZ best variational -0.529024 ○ HF Motta et al. (2017)
best projected -0.55142(2) ph-AFQMC Motta et al. (2017)
best approximate -0.5509443 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2.4, basis-free best variational -0.550876(9) VMC (SJ) Motta et al. (2017)
best projected -0.55248(2) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 2.4, STO-6G best variational -0.5231183 ○ DMRG Motta et al. (2017)
best projected -0.523325 ○ DMET Motta et al. (2017)
best approximate -0.5239338 ○ RCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2.8, cc-pV5Z best variational -0.5183556 ○ HF Motta et al. (2017)
H30 chain, open, R = 2.8, cc-pVDZ best variational -0.5340762 ○ DMRG Motta et al. (2017)
best projected -0.5347214 ○ SEET Motta et al. (2017)
best approximate -0.5327924 ○ UCCSD(T) Motta et al. (2017)
H30 chain, open, R = 2.8, cc-pVQZ best variational -0.5183116 ○ HF Motta et al. (2017)
best projected -0.53788(4) ph-AFQMC Motta et al. (2017)
H30 chain, open, R = 2.8, cc-pVTZ best variational -0.5181643 ○ HF Motta et al. (2017)
best projected -0.53718(3) ph-AFQMC Motta et al. (2017)
H30 chain, open, R = 2.8, basis-free best variational -0.536326(9) VMC (SJ) Motta et al. (2017)
best projected -0.53821(2) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 2.8, STO-6G best variational -0.5054037 ○ DMRG Motta et al. (2017)
best projected -0.5055314 ○ DMET Motta et al. (2017)
best approximate -0.5037865 ○ UCCSD(T) Motta et al. (2017)
H30 chain, open, R = 3.2, cc-pV5Z best variational -0.5102735 ○ HF Motta et al. (2017)
H30 chain, open, R = 3.2, cc-pVDZ best variational -0.5216948 ○ DMRG Motta et al. (2017)
best projected -0.5240882 ○ SEET Motta et al. (2017)
best approximate -0.5205262 ○ UCCSD(T) Motta et al. (2017)
H30 chain, open, R = 3.2, cc-pVQZ best variational -0.5102287 ○ HF Motta et al. (2017)
best projected -0.52512(7) ph-AFQMC Motta et al. (2017)
H30 chain, open, R = 3.2, cc-pVTZ best variational -0.5100848 ○ HF Motta et al. (2017)
best projected -0.52443(4) ph-AFQMC Motta et al. (2017)
H30 chain, open, R = 3.2, basis-free best variational -0.523410(9) VMC (SJ) Motta et al. (2017)
best projected -0.52555(2) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 3.2, STO-6G best variational -0.4913033 ○ DMRG Motta et al. (2017)
best projected -0.4914582 ○ SEET Motta et al. (2017)
best approximate -0.4900449 ○ UCCSD(T) Motta et al. (2017)
H30 chain, open, R = 3.6, cc-pV5Z best variational -0.5053753 ○ HF Motta et al. (2017)
H30 chain, open, R = 3.6, cc-pVDZ best variational -0.512651 ○ DMRG Motta et al. (2017)
best projected -0.5128862 ○ DMET Motta et al. (2017)
best approximate -0.511785 ○ UCCSD(T) Motta et al. (2017)
H30 chain, open, R = 3.6, cc-pVQZ best variational -0.5053287 ○ HF Motta et al. (2017)
best projected -0.5162413 ○ DMET Motta et al. (2017)
H30 chain, open, R = 3.6, cc-pVTZ best variational -0.5051879 ○ HF Motta et al. (2017)
best projected -0.5154642 ○ DMET Motta et al. (2017)
H30 chain, open, R = 3.6, basis-free best variational -0.513577(9) VMC (SJ) Motta et al. (2017)
best projected -0.51601(3) LR-DMC (LDA determinant) Motta et al. (2017)
H30 chain, open, R = 3.6, STO-6G best variational -0.4820203 ○ DMRG Motta et al. (2017)
best projected -0.4828246 ○ SEET Motta et al. (2017)
best approximate -0.4812442 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1, cc-pV5Z best variational -0.3930718 ○ HF Motta et al. (2017)
H50 chain, open, R = 1, cc-pVDZ best variational -0.388254 ○ DMRG Motta et al. (2017)
best projected -0.38822(2) ph-AFQMC Motta et al. (2017)
best approximate -0.3882394 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1, cc-pVQZ best variational -0.3909264 ○ HF Motta et al. (2017)
best projected -0.4169616 ○ RCCSD Motta et al. (2017)
best approximate -0.418261 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1, cc-pVTZ best variational -0.3867182 ○ HF Motta et al. (2017)
best projected -0.41352(4) ph-AFQMC Motta et al. (2017)
best approximate -0.4133358 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1, basis-free best variational -0.41856(3) VMC (SJ) Motta et al. (2017)
best projected -0.42197(3) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 1, STO-6G best variational -0.3456814 ○ LDMRG Hachmann et al. (2006)
best projected -0.3466732 ○ DMET Motta et al. (2017)
best approximate -0.345728 ○ GW Motta et al. (2017)
H50 chain, open, R = 1.2, cc-pV5Z best variational -0.4724546 ○ HF Motta et al. (2017)
H50 chain, open, R = 1.2, cc-pVDZ best variational -0.486182 ○ DMRG Motta et al. (2017)
best projected -0.48637(1) ph-AFQMC Motta et al. (2017)
best approximate -0.4860532 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.2, cc-pVQZ best variational -0.471144 ○ HF Motta et al. (2017)
best projected -0.49888(3) ph-AFQMC Motta et al. (2017)
best approximate -0.4983418 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.2, cc-pVTZ best variational -0.4700515 ○ HF Motta et al. (2017)
best projected -0.49746(4) ph-AFQMC Motta et al. (2017)
best approximate -0.4971284 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.2, basis-free best variational -0.49748(1) VMC (SJ) Motta et al. (2017)
best projected -0.49913(4) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 1.2, STO-6G best variational -0.458953 ○ LDMRG Hachmann et al. (2006)
best projected -0.4599375 ○ DMET Motta et al. (2017)
best approximate -0.4588914 ○ CCSD(T) Hachmann et al. (2006)
H50 chain, open, R = 1.4, cc-pV5Z best variational -0.5142633 ○ HF Motta et al. (2017)
H50 chain, open, R = 1.4, cc-pVDZ best variational -0.5331854 ○ DMRG Motta et al. (2017)
best projected -0.5342916 ○ DMET Motta et al. (2017)
best approximate -0.5330286 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.4, cc-pVQZ best variational -0.5141705 ○ HF Motta et al. (2017)
best projected -0.5401476 ○ RCCSD Motta et al. (2017)
best approximate -0.5411192 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.4, cc-pVTZ best variational -0.5138868 ○ HF Motta et al. (2017)
best projected -0.54063(3) ph-AFQMC Motta et al. (2017)
best approximate -0.540299 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.4, basis-free best variational -0.53996(2) VMC (SJ) Motta et al. (2017)
best projected -0.54153(2) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 1.4, STO-6G best variational -0.5118756 ○ LDMRG Hachmann et al. (2006)
best projected -0.5127902 ○ DMET Motta et al. (2017)
best approximate -0.5117824 ○ CCSD(T) Hachmann et al. (2006)
H50 chain, open, R = 1.6, cc-pV5Z best variational -0.5332496 ○ HF Motta et al. (2017)
H50 chain, open, R = 1.6, cc-pVDZ best variational -0.5307409 ○ HF Motta et al. (2017)
best projected -0.5548843 ○ DMET Motta et al. (2017)
best approximate -0.5535398 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.6, cc-pVQZ best variational -0.5331783 ○ HF Motta et al. (2017)
best projected -0.558395 ○ RCCSD Motta et al. (2017)
best approximate -0.5594386 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.6, cc-pVTZ best variational -0.5329572 ○ HF Motta et al. (2017)
best projected -0.55895(3) ph-AFQMC Motta et al. (2017)
best approximate -0.5587018 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.6, basis-free best variational -0.55836(1) VMC (SJ) Motta et al. (2017)
best projected -0.55992(2) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 1.6, STO-6G best variational -0.5343888 ○ LDMRG Hachmann et al. (2006)
best projected -0.5351831 ○ DMET Motta et al. (2017)
best approximate -0.5342628 ○ CCSD(T) Hachmann et al. (2006)
H50 chain, open, R = 1.8, cc-pV5Z best variational -0.5393799 ○ HF Motta et al. (2017)
H50 chain, open, R = 1.8, cc-pVDZ best variational -0.560418 ○ DMRG Motta et al. (2017)
best projected -0.5615634 ○ DMET Motta et al. (2017)
best approximate -0.5601304 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.8, cc-pVQZ best variational -0.5393155 ○ HF Motta et al. (2017)
best projected -0.56515(3) ph-AFQMC Motta et al. (2017)
best approximate -0.564877 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.8, cc-pVTZ best variational -0.5391208 ○ HF Motta et al. (2017)
best projected -0.56451(4) ph-AFQMC Motta et al. (2017)
best approximate -0.5641164 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 1.8, basis-free best variational -0.56381(1) VMC (SJ) Motta et al. (2017)
best projected -0.56543(2) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 1.8, STO-6G best variational -0.540773 ○ LDMRG Hachmann et al. (2006)
best projected -0.5414071 ○ DMET Motta et al. (2017)
best approximate -0.540629 ○ CCSD(T) Hachmann et al. (2006)
H50 chain, open, R = 2, cc-pV5Z best variational -0.5387831 ○ HF Motta et al. (2017)
H50 chain, open, R = 2, cc-pVDZ best variational -0.5376519 ○ HF Motta et al. (2017)
best projected -0.560789 ○ DMET Motta et al. (2017)
best approximate -0.5593002 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2, cc-pVQZ best variational -0.5387247 ○ HF Motta et al. (2017)
best projected -0.56380(3) ph-AFQMC Motta et al. (2017)
best approximate -0.5634712 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2, cc-pVTZ best variational -0.5385504 ○ HF Motta et al. (2017)
best projected -0.56316(5) ph-AFQMC Motta et al. (2017)
best approximate -0.5626926 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2, basis-free best variational -0.56242(1) VMC (SJ) Motta et al. (2017)
best projected -0.56409(2) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 2, STO-6G best variational -0.5385218 ○ DMRG Motta et al. (2017)
best projected -0.5389803 ○ DMET Motta et al. (2017)
best approximate -0.538418 ○ CCSD(T) Hachmann et al. (2006)
H50 chain, open, R = 2.4, cc-pV5Z best variational -0.5294429 ○ HF Motta et al. (2017)
H50 chain, open, R = 2.4, cc-pVDZ best variational -0.5484576 ○ DMRG Motta et al. (2017)
best projected -0.549566 ○ DMET Motta et al. (2017)
best approximate -0.5481804 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2.4, cc-pVQZ best variational -0.5293962 ○ HF Motta et al. (2017)
best projected -0.5505126 ○ RCCSD Motta et al. (2017)
best approximate -0.5518596 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2.4, cc-pVTZ best variational -0.5292454 ○ HF Motta et al. (2017)
best projected -0.55145(4) ph-AFQMC Motta et al. (2017)
best approximate -0.5510824 ○ RCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2.4, basis-free best variational -0.55049(1) VMC (SJ) Motta et al. (2017)
best projected -0.55262(3) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 2.4, STO-6G best variational -0.5232114 ○ LDMRG Hachmann et al. (2006)
best projected -0.5234051 ○ DMET Motta et al. (2017)
best approximate -0.521806 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2.8, cc-pV5Z best variational -0.518544 ○ HF Motta et al. (2017)
H50 chain, open, R = 2.8, cc-pVDZ best variational -0.51777 ○ HF Motta et al. (2017)
best projected -0.5352079 ○ DMET Motta et al. (2017)
best approximate -0.5329892 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 2.8, cc-pVQZ best variational -0.5185002 ○ HF Motta et al. (2017)
best projected -0.53798(3) ph-AFQMC Motta et al. (2017)
H50 chain, open, R = 2.8, cc-pVTZ best variational -0.5183529 ○ HF Motta et al. (2017)
best projected -0.53742(2) ph-AFQMC Motta et al. (2017)
H50 chain, open, R = 2.8, basis-free best variational -0.53563(1) VMC (SJ) Motta et al. (2017)
best projected -0.53834(3) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 2.8, STO-6G best variational -0.505496 ○ LDMRG Hachmann et al. (2006)
best projected -0.5056322 ○ DMET Motta et al. (2017)
best approximate -0.503953 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 3.2, cc-pV5Z best variational -0.5103961 ○ HF Motta et al. (2017)
H50 chain, open, R = 3.2, cc-pVDZ best variational -0.5217914 ○ DMRG Motta et al. (2017)
best projected -0.5226823 ○ DMET Motta et al. (2017)
best approximate -0.5206612 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 3.2, cc-pVQZ best variational -0.5103515 ○ HF Motta et al. (2017)
H50 chain, open, R = 3.2, cc-pVTZ best variational -0.5102075 ○ HF Motta et al. (2017)
best projected -0.52450(4) ph-AFQMC Motta et al. (2017)
H50 chain, open, R = 3.2, basis-free best variational -0.52221(2) VMC (SJ) Motta et al. (2017)
best projected -0.52570(4) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 3.2, STO-6G best variational -0.4913656 ○ DMRG Motta et al. (2017)
best projected -0.4916637 ○ SEET Motta et al. (2017)
best approximate -0.4901495 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 3.6, cc-pV5Z best variational -0.5054446 ○ HF Motta et al. (2017)
H50 chain, open, R = 3.6, cc-pVDZ best variational -0.5046794 ○ HF Motta et al. (2017)
best projected -0.5134833 ○ DMET Motta et al. (2017)
best approximate -0.5118654 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 3.6, cc-pVQZ best variational -0.5053981 ○ HF Motta et al. (2017)
H50 chain, open, R = 3.6, cc-pVTZ best variational -0.5052571 ○ HF Motta et al. (2017)
best projected -0.5156009 ○ DMET Motta et al. (2017)
H50 chain, open, R = 3.6, basis-free best variational -0.51192(1) VMC (SJ) Motta et al. (2017)
best projected -0.51616(7) LR-DMC (LDA determinant) Motta et al. (2017)
H50 chain, open, R = 3.6, STO-6G best variational -0.4820554 ○ LDMRG Hachmann et al. (2006)
best projected -0.4831221 ○ SEET Motta et al. (2017)
best approximate -0.4813012 ○ UCCSD(T) Motta et al. (2017)
H50 chain, open, R = 4.2, STO-6G best variational -0.4749942 ○ LDMRG Hachmann et al. (2006)
best approximate -0.4302988 ○ MP2 Hachmann et al. (2006)
H70 chain, open, R = 1, STO-6G best projected -0.34303(1) ph-AFQMC Motta et al. (2017)
H70 chain, open, R = 1.4, STO-6G best projected -0.511254(9) ph-AFQMC Motta et al. (2017)
H70 chain, open, R = 1.8, STO-6G best projected -0.54073(1) ph-AFQMC Motta et al. (2017)
H70 chain, open, R = 2.8, STO-6G best projected -0.50560(1) ph-AFQMC Motta et al. (2017)
H82 chain, open, R = 1, basis-free best variational -0.41649(2) VMC (SJ) Motta et al. (2017)
best projected -0.42018(3) LR-DMC (LDA determinant) Motta et al. (2017)
H82 chain, open, R = 1.2, basis-free best variational -0.49544(1) VMC (SJ) Motta et al. (2017)
best projected -0.49896(7) LR-DMC (LDA determinant) Motta et al. (2017)
H102 chain, open, R = 1, basis-free best variational -0.41616(2) VMC (SJ) Motta et al. (2017)
best projected -0.41967(4) LR-DMC (LDA determinant) Motta et al. (2017)
H102 chain, open, R = 1, STO-6G best projected -0.34087(1) ph-AFQMC Motta et al. (2017)
H102 chain, open, R = 1.2, basis-free best variational -0.49576(1) VMC (SJ) Motta et al. (2017)
best projected -0.49844(4) LR-DMC (LDA determinant) Motta et al. (2017)
H102 chain, open, R = 1.4, STO-6G best projected -0.51125(1) ph-AFQMC Motta et al. (2017)
H102 chain, open, R = 1.8, basis-free best variational -0.563316(7) VMC (SJ) Motta et al. (2017)
best projected -0.56538(1) LR-DMC (LDA determinant) Motta et al. (2017)
H102 chain, open, R = 1.8, STO-6G best projected -0.54069(2) ph-AFQMC Motta et al. (2017)
H102 chain, open, R = 2.8, STO-6G best projected -0.50565(2) ph-AFQMC Motta et al. (2017)
Hydrogen sheet: 1 instances, energies as E/N (Ha)
instance value energy method code
H4 sheet (2x2), open, R = 2.4, basis-free best variational -0.52710(7) VMC (JAGP) Genovese et al. (2019)
best projected -0.52812(5) LR-DMC (JAGP) Genovese et al. (2019)

Details

Every row has a bound_type that says what kind of number the energy is
(RULES.md §4).

Bold marks the record. RULES.md §6 says how it is chosen.

○ marks a row where no error bar and no energy variance was found in the source.
† marks a sampled energy with a variance but no error bar. Both rows stay in rank
order. Error metrics defines the markers.

The code column links the code that produced a result, where its authors published it: the
place to start when you want to rerun it. For a row QMBL computed, "rerun (QMBL code)" links the
command, the commit and the package versions it ran with. Where the authors published no code
of their own, a muted "uses …" names the library they used, if their paper says. An empty
cell means that no source read so far names the code or a library.
How the links were found.

Rules: RULES.md. Units, conventions, error metrics, provenance and defects:
DATA.md.

Citing

T. Zerweck and J. Carrasquilla, QMBL: the Quantum Many-Body Leaderboard,
arXiv:2610.22387 (2026).

To cite the data itself, use the Zenodo concept DOI, which resolves to the latest release: 10.5281/zenodo.22753734.

Contributing

To add an energy, use the new result form.
To add an instance QMBL does not have yet, a lattice model or an electron-gas cell, use the
new instance form.
To correct a row or comment on it, click the pencil at the end of the row on
qmbl.org/instances; it opens the
about-a-row form with the row filled in. Be specific and technical
(RULES.md §10). A sampled energy without an
error bar is marked †. Send the error bar so the row can be compared with its
neighbours.

CONTRIBUTING.md gives the details: what happens after you submit, how
to change the code, and how AI systems submit.

Contributors

Everyone whose issue or pull request leads to a change is listed here.

License

Apache-2.0. The data tables are freely reusable with attribution.

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