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Hubbard rectangular 6x48, U = 12, n = 0.875

Best values (rules §6)

best variational -0.62556(3) VMC (Jastrow + BF)
Wu et al. (2024) · the lowest unflagged variational energy, a strict variational bound
best projected -0.63217(2) FN-GFMC (Jastrow + BF)
Wu et al. (2024) · the lowest unflagged projected energy, a projected estimate, which depends on its node or constraint

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 = 12, N↑ = N↓ = 126 on 288 sites.

lattice
rectangular-6x48
sites
288
boundary
periodic
Nf
126
U
12
energies
6

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).

Strict variational upper bounds (4)

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
-0.62556best variational 0 3.5e-5 2.15e+1 7.6e-3 VMC (Jastrow + BF)
VarBench reference run
Wu et al. (2024) run script 2024
-0.6255tied with best variational at 2σ 5.6e-5 n/a n/a n/a VMC (Jastrow + BF)
peer reviewed
Marino et al. (2022) 2022
-0.6227 2.9e-3 n/a n/a n/a VMC (Jastrow + BF)
peer reviewed
Marino et al. (2022) 2022
-0.62226 3.3e-3 2.8e-5 3.49e+1 1.2e-2 VMC (Jastrow + BF)
VarBench reference run
Wu et al. (2024) run script 2024

Projected or fixed-node estimates (2)

Variational only within a constraint: fixed-node, constrained-path, GFMC on a trial state. Each depends on its node or constraint, so two of them are not cleanly comparable to each other or to strict bounds.

E/sitedistance to class bestσVar(E)V-score methodsourcecodeyearcomment
-0.63217best projected 0 1.7e-5 n/a n/a FN-GFMC (Jastrow + BF)
VarBench reference run
Wu et al. (2024) run script 2024
-0.62965 2.5e-3 1.4e-5 n/a n/a FN-GFMC (Jastrow + BF)
VarBench reference run
Wu et al. (2024) run script 2024

How these numbers were read

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

-0.63217(2), FN-GFMC (Jastrow + BF)

Checked 2026-09-29 · run script scripts/Hubbard/rectangular-6x48_288_P_126_12/FN-stripes/fn_hubbard.sh with datprep.d and datasfn.d, programs/vmc_hubbard/{Prep_stripes_wf.f, Main_stripes_wf.f, Energy.f90, Variance.f} read (varbench/methods@ed31bb0); VarBench history (git clone of github.com/varbench/varbench, partial, read with git log --follow; old names normalised)

Reported as. -182.065 | 0.005 | (VarBench upload by L. F. Tocchio)

48 x 6 torus (the compiled nx = 48, nh = 288; ny = nh/nx = 6), periodic in both directions, t = 1, no t', U = 12 with U n_up n_dn (no constant shift: the diagonal energy is U per doubly occupied site, Main_*_wf.f 'diag(k)=diag(k)-U'), N_up = nelup = 126, N_dn = 288 - neldo = 126 (particle-hole transformed down spins, as the code states for iopt >= 0): the instance. Stripe wavelength 6 as printed. Lattice fixed-node GFMC (gamma = 0) on the VMC state: projected is right; its trial energy etry agrees with the result per site. The M3 flag (FN below the best variational bound) is expected: FN improves on its own trial state. No output log in the repository (scope config). FN not printed in the papers.

-0.62556(3), VMC (Jastrow + BF)

Checked 2026-09-29 · run script scripts/Hubbard/rectangular-6x48_288_P_126_12/VMC-stripes/vmc_hubbard.sh with datprep.d and datasvmc.d, programs/vmc_hubbard/{Prep_stripes_wf.f, Main_stripes_wf.f, Energy.f90, Variance.f} read (varbench/methods@ed31bb0); VarBench history (git clone of github.com/varbench/varbench, partial, read with git log --follow; old names normalised)

Reported as. -180.16 | 0.01 | 21.5 (VarBench upload by L. F. Tocchio)

48 x 6 torus (the compiled nx = 48, nh = 288; ny = nh/nx = 6), periodic in both directions, t = 1, no t', U = 12 with U n_up n_dn (no constant shift: the diagonal energy is U per doubly occupied site, Main_*_wf.f 'diag(k)=diag(k)-U'), N_up = nelup = 126, N_dn = 288 - neldo = 126 (particle-hole transformed down spins, as the code states for iopt >= 0): the instance. Stripe wavelength 6 as printed. Jastrow + backflow VMC: variational is right. The M11 margins over the uniform state are the physics of the stripe state, not an error. No output log in the repository (scope config). Published corroboration: arXiv:2111.04623v4 (SciPost Phys. 12, 180 (2022)) Table 2, U/t = 12, t'/t = 0, Lx = 48: '-0.6255 (λ = 6)' ('The error bar on the energy is always smaller than 10^-4'); stored -180.16/288 = -0.625556 differs by 5.6e-5.

-0.6255, VMC (Jastrow + BF)

Checked 2026-10-07 · source text of arXiv:2111.04623 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. -0.6255

Table 2 (U/t = 12, Lx = 48), row t'/t = 0, column E_stripe (λ = 6); no per-value error bar | Energy per site in units of t on Lx x 6 ladders with 'periodic boundary conditions along both the x and the y directions', hole doping 1/8 (n = 7/8). 'The error bar on the energy is always smaller than 10^-4' is one statement for the whole table, not a per-value sigma.

-0.6227, VMC (Jastrow + BF)

Checked 2026-10-07 · source text of arXiv:2111.04623 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. -0.6227

Table 2 (U/t = 12, Lx = 48), row t'/t = 0, column E_uniform; no per-value error bar | Energy per site in units of t on Lx x 6 ladders with 'periodic boundary conditions along both the x and the y directions', hole doping 1/8 (n = 7/8). 'The error bar on the energy is always smaller than 10^-4' is one statement for the whole table, not a per-value sigma.

Coverage

Newest published number here: 2024.

This instance as data

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