QMBLthe quantum many-body leaderboard

All instances / Hubbard

Hubbard square 4x4, U = 3.59381366, n = 0.5

Exact energy and best values (rules §6)

exact -1.1061269 ED
Moreno et al. (2022) · the instance is solved
best variational -1.105848(3) VMC (HFDS)
Moreno et al. (2022) · the lowest unflagged variational energy, a strict variational bound

Energies as E/site. Classes are different claims and are not ranked against each other.

The Hamiltonian

H = −t ∑⟨ij⟩,σ (c†iσcjσ + h.c.) + U ∑i ni↑ni↓

t = 1, U = 3.59381366, N↑ = N↓ = 4 on 16 sites.

Upstream this instance is Hubbard/square_16_P_4_3.5981. The name's 3.5981 has two digits swapped: the coupling of this Hamiltonian is 3.59381366 (10^(5/9)). The exact diagonalization, -17.698030018702067, is the ground state there; at U = 3.5981 the ground state is 1.79e-3 higher, so the stored exact energy sat below the ground state of the instance as named. Evidence: checks/hubbard-u-labels.

lattice
square
sites
16
boundary
periodic
Nf
4
U
3.59381366
energies
16

Stored as a total energy; quoted here as E/site, which is what the papers report (how the conversion works).

Every published energy

Grouped by what the number is. The exact energy comes first where there is one; in every other group the lowest unflagged energy is its best value, and each row's distance is to that best (rules §6).

Numerically exact (1)

Exact diagonalization, an exact solution, or sign-problem-free QMC where that is established. An exact energy is shown first, before the best of each other class. QMC is exact only within its error bar, which it must state, and reads exact (stochastic); an exact diagonalization outranks it. For a diagonalization resolved by symmetry sector only the ground state's sector is listed; the lowest energies of the other sectors are the instance's spectrum, in its JSON, and are not shown as the exact energy.

E/sitedistance to class bestσVar(E)V-score methodsourcecodeyearcomment
-1.1061269exact 0 n/a n/a n/a ED Moreno et al. (2022) 2022

Strict variational upper bounds (15)

Energies that a variational state reached (VMC, DMRG and MPS at finite bond dimension, PEPS, NQS, VQE). Each is an upper bound on the ground-state energy.

E/sitedistance to class bestσVar(E)V-score methodsourcecodeyearcomment
-1.105848best variational 0 2.5e-6 3.30e-2 5.8e-4 VMC (HFDS) Moreno et al. (2022) uses NetKet 2022
-1.10581tied with best variational at 2σ 4.2e-5 5.0e-5 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.10578tied with best variational at 2σ 6.7e-5 3.7e-5 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.10561 2.4e-4 2.5e-5 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.105581 2.7e-4 6.3e-6 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.105239 6.1e-4 5.6e-6 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.103532 2.3e-3 4.4e-6 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.102726 3.1e-3 5.6e-6 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.101150 4.7e-3 6.3e-6 n/a n/a VMC (RBM)
peer reviewed
Moreno et al. (2022) 2022
-1.098930 6.9e-3 5.0e-6 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.098918 6.9e-3 5.6e-6 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.09700 8.8e-3 6.3e-5 n/a n/a VMC (SJ)
peer reviewed
Moreno et al. (2022) 2022
-1.09679 9.1e-3 1.9e-5 n/a n/a VMC (SJ)
peer reviewed
Moreno et al. (2022) 2022
-1.05434 5.2e-2 1.3e-5 n/a n/a VMC (HFDS)
peer reviewed
Moreno et al. (2022) uses NetKet 2022
-1.053 5.3e-2 5.0e-3 n/a n/a HF
peer reviewed
Moreno et al. (2022) 2022

How these numbers were read

Where each number below was read, and how it was checked.

-1.1061269, ED

Checked 2026-09-16 · recomputed: Lanczos ED over the full fixed-(N_up, N_dn) space by two independent codes (checks/hubbard-u-labels/)

Reported as. -17.698030018702013 (ed_check.py) | -17.69803001870263 (ed_lib.mjs)

Reproduced at the grid U the instance now carries, not at the U of VarBench's name (relabels.mjs).

-1.105848(3), VMC (HFDS)

Checked 2026-09-29 · PNAS 119(32), e2122059119 (2022), SI Appendix PDF (PMC9371695; sources/pnas.2122059119.sapp.PMC9371695.pdf, sha256 c6e62d9c...), pypdf layout mode, re-extracted 2026-09-29 (byte-identical to the earlier extraction); same cell read in arXiv:2111.10420v2 (18 Jun 2022) Appendix H (sources/2111.10420v2.pdf, pypdf layout)

Reported as. -17.69357(4) (total energy, units of t)

Record row (best variational bound; the instance record is the ED row, 0.00446 below). 4 x 4 torus, n = 1/2 = 4 + 4 at zero magnetization ('In all cases we focus on the zero magnetization and fixed visible- and hidden-particle subspaces', p. 5), t = 1, U n_up n_dn with no shift (Eq. 1). U '3.6' is the grid value 3.59381366 (the paper's own ED in this row is the ground state there). N~ = 8 (main Fig. 3 caption, 'Average physical site occupation is n = 1/2 and N~ = 8'), single hidden layer, alpha = 32: method string and detail right. Variational VMC bound, own computation. Stored sigma equals the printed bar. energy_variance 0.033 is the upload's (7f646d3: -17.69357 | 0.00004 | 0.033(2)); not printed as a number. Venue PNAS, peer reviewed ('Edited by Angel Rubio ... received December 6, 2021; accepted June 28, 2022'; 'This article is a PNAS Direct Submission'); the imported row carries no peer_reviewed field (loader-level, see report). No duplicate (the only other row is the ED).

-1.10581(5), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.6929(8)

Appendix H Table I, U=3.6, column HFDS alpha=16; sources/2111.10420.txt line 1177; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29 | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.10578(4), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.6925(6)

Appendix H Table I, U=3.6, column HFDS alpha=8; sources/2111.10420.txt line 1177; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#65: sigma 0.000608 -> 0.0006 (The table prints totals, so the bar is 0.0006 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 1.3%. Same fix as the trailing-float-noise ruling: store sigma_per_s) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.10561(3), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.6897(4)

Appendix H Table I, U=3.6, column HFDS alpha=4; sources/2111.10420.txt line 1177; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29 | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.105581(6), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.6893(1)

Appendix H Table I, U=3.6, column HFDS alpha=2; sources/2111.10420.txt line 1177; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#63: sigma 0.0001008 -> 0.0001 (The table prints totals, so the bar is 0.0001 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 0.8%. Same fix as the trailing-float-noise ruling: store sigma_per_s) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.105239(6), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.68383(9)

Appendix H Table I, U=3.6, column HFDS alpha=1; sources/2111.10420.txt line 1177; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#62: sigma 0.0000896 -> 0.00009 (The table prints totals, so the bar is 0.00009 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 0.4%. Same fix as the trailing-float-noise ruling: store sigma_per_) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.103532(4), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.65651(7)

Appendix H Table I, U=3.6, column HFDS alpha=0.5; sources/2111.10420.txt line 1177; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#61: sigma 0.0000704 -> 0.00007 (The table prints totals, so the bar is 0.00007 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 0.6%. Same fix as the trailing-float-noise ruling: store sigma_per_) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.102726(6), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.64362(9)

Appendix H Table II, U=3.6, row Unrestricted hid. spin(RBM); sources/2111.10420.txt line 1202; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#75: sigma 0.0000896 -> 0.00009 (The table prints totals, so the bar is 0.00009 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 0.4%. Same fix as the trailing-float-noise ruling: store sigma_per_) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.101150(6), VMC (RBM)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.6184(1)

Appendix H Table II, U=3.6, row USD (RBM); sources/2111.10420.txt line 1197; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#71: sigma 0.0001008 -> 0.0001 (The table prints totals, so the bar is 0.0001 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 0.8%. Same fix as the trailing-float-noise ruling: store sigma_per_s) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.098930(5), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.58288(8)

Appendix H Table II, U=3.6, row Unrestricted hidden spin; sources/2111.10420.txt line 1199; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29 | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.098918(6), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.58269(9)

Appendix H Table II, U=3.6, row Gutzwiller inspired CF; sources/2111.10420.txt line 1198; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#72: sigma 0.0000896 -> 0.00009 (The table prints totals, so the bar is 0.00009 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 0.4%. Same fix as the trailing-float-noise ruling: store sigma_per_) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.09700(6), VMC (SJ)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.552(1)

Appendix H Table II, U=3.6, row USD (Gutzwiller); sources/2111.10420.txt line 1195; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#69: sigma 0.001008 -> 0.001 (The table prints totals, so the bar is 0.001 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 0.8%. Same fix as the trailing-float-noise ruling: store sigma_per_si) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.09679(2), VMC (SJ)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -17.5487(3)

Appendix H Table II, U=3.6, row USD (Jastrow); sources/2111.10420.txt line 1196; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#70: sigma 0.000304 -> 0.0003 (The table prints totals, so the bar is 0.0003 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 1.3%. Same fix as the trailing-float-noise ruling: store sigma_per_s) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.05434(1), VMC (HFDS)

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -16.8694(2)

Appendix H Table II, U=3.6, row Jastrow inspired CF; sources/2111.10420.txt line 1200; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29; qmbl-verify 2026-10-19 SP2-arxiv-2111-10420#74: sigma 0.000208 -> 0.0002 (The table prints totals, so the bar is 0.0002 as printed; the round trip through a rounded per-site sigma inflates or shrinks it by 4.0%. Same fix as the trailing-float-noise ruling: store sigma_per_s) | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

-1.053(5), HF

Checked 2026-10-16 · source text of arXiv:2111.10420 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; single reading

Reported as. -16.85(8)

Appendix H Table II, U=3.6, row USD; sources/2111.10420.txt line 1194; version read: arXiv:2111.10420v2 text, Appendix H (sources/2111.10420.txt); the PNAS SI (Cloudflare 403 on 2026-10-16) was read for this paper's earlier rows on 2026-09-29 | Eq. (1): H = -sum t_ij (c+c + h.c.) + U sum n_up n_dn, t = 1. Tables I-III print totals on the 4x4 torus (ED -17.698 on 16 sites); Tables IV and V print 'energy per site'. The rounded U of the tables (0.6, 2.15, 3.6, 7.75) are the grid 10^(k/9): QMBL's ED at U = 0.59948425 gives -19.47476333 and at 2.15443469 (n = 1/2) -18.40532088, the printed ED values, against -19.47434179 at U = 0.6 and -18.40534078 at U = 2.1544 (checks/hubbard-u-labels/results-2026-10-16/, run_fermions.mjs).

Coverage

Newest published number here: 2022. Literature last checked 2026-09-15 (citation screen of Robledo Moreno et al. 2022 (PNAS, HFDS): citing works from OpenAlex and Semantic Scholar (scripts/cited_by.mjs)): 29 papers read, 0 of them with an energy on this page.

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