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All instances / Heisenberg

Heisenberg square, 38 sites

Exact energy and best values (rules §6)

exact -0.6779156 ED
Richter et al. (2004) · the instance is solved

Energies as E/N (S.S). Classes are different claims and are not ranked against each other.

The Hamiltonian

H = ∑⟨ij⟩ σi·σj

Nearest-neighbour Heisenberg antiferromagnet, J = 1, written with Pauli matrices.

lattice
square
sites
38
boundary
periodic
energies
1

Stored as a total energy; quoted here as E/N (S.S), 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/N (S.S)distance to class bestσVar(E)V-score methodsourcecodeyearcomment
-0.6779156exact 0 n/a n/a n/a ED
preprint
Richter et al. (2004) 2004

How these numbers were read

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

-0.6779156, ED

Checked 2026-10-24 · arXiv:cond-mat/0412662: publisher PDF (Springer, scanned) Table 2.1, read from the page image rendered at 200 %; checked against the arXiv text (pypdf layout and plain modes); no LLM transcription of numbers; single reading + page-image check

Reported as. −25.7607925

Table 2.1 (p. 102), row N = 38, edge vectors (1, 7), (-5, 3), column E0. No other row on this cluster. | Spin-1/2 Heisenberg antiferromagnet H = J sum_<ij> S_i . S_j on the square lattice, J = 1, periodic boundaries on the finite lattice defined by the two edge vectors printed in the row (Betts construction, Sec. 2.4.1); E0 is the total singlet ground-state energy in S.S units, stored as the Pauli total 4 E0. Version read: publisher PDF (Springer, a scan), Table 2.1 on p. 102 read from the page image; identical to Table 1 of the arXiv text cond-mat/0412662. Peer review: a chapter of an edited lecture-notes volume, not a refereed journal.

Coverage

Newest published number here: 2004.

This instance as data

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