Heisenberg1D — model index

The spin-$\tfrac12$ antiferromagnetic Heisenberg chain — the Bethe-ansatz-integrable model of quantum magnetism, gapless with an $SU(2)_1$ WZW critical point ($c = 1$).

\[H = J\sum_{\langle i,j\rangle} \mathbf{S}_i \cdot \mathbf{S}_j, \qquad J > 0\]

Provisional v2 view — RES not wired

Generated by docs/atlas/generate.jl — a pure VIEW over the *_registry.jl claims + the static test/INVENTORY.jsonl AST scan. No test is executed and no src is run; test/INVENTORY.jsonl is regenerated in-place (idempotently) from that static scan; fetch/@register untouched. Assurance labels are PROVISIONAL: residuals / confidence are not shown yet (RES not wired). Badges reflect the committed test AST, not the latest CI run — a hub can read green while its @test is red between regenerations. @sweep = a graceful regime-resolution gap, not card omission.

All (Quantity, BC) hubs src claims for Heisenberg1D. Cells link to the per-hub card; = not yet implemented at that BC. The shape of the matrix is the gap visualisation: empty cells are where physics could be added next.

Convention

FieldValue
HamiltonianSpin S (this file)
ObservableSpin S (QAtlas-wide spin convention; see docs/src/conventions.md)

Coverage

LevelCount
🟣 universality-corroborated0
🟢 corroborated-at-p13
🔵 coherent4
⚪ cited-only0
🟠 uncorroborated-but-feasible11
total claimed hubs28

Methods (from @register, derived): analytic, bethe_ansatz, cft, cft_low_T, delegation, dense_ed, muller_ansatz

Quantity × BC matrix

QuantityOBCPBCInfinite
ConformalTower🟠 hub
Energy🟢 hub
EnergyLocal🟠 hub
FreeEnergy🟢 hub🟠 hub
GroundStateEnergyDensity🟢 hub
LuttingerParameter🔵 hub
MagnetizationX🔵 hub
MagnetizationXLocal🟠 hub
MagnetizationY🔵 hub
MagnetizationYLocal🟠 hub
MagnetizationZ🔵 hub
MagnetizationZLocal🟠 hub
MassGap🟢 hub🟢 hub
RenyiEntropy🟢 hub🟠 hub
SpecificHeat🟢 hub🟠 hub
SusceptibilityXX🟢 hub
SusceptibilityYY🟢 hub
SusceptibilityZZ🟢 hub
ThermalEntropy🟢 hub🟠 hub
UniversalityClass🟠 hub
VonNeumannEntropy🟢 hub🟠 hub
ZZStructureFactor🟢 hub

Derivation notes

Matched by filename substring (no annotation; substrate-derived):

References

Papers cited by this model's @register cards. The full numbered list is on the Reference List.

[82]
I. Affleck. Universal term in the free energy at a critical point and the conformal anomaly. Physical Review Letters 56, 746–748 (1986).
[83]
I. Affleck. Quantum spin chains and the Haldane gap. Journal of Physics: Condensed Matter 1, 3047–3072 (1989).
[84]
H. Bethe. Zur Theorie der Metalle. Zeitschrift f�r Physik 71, 205–226 (1931).
[31]
H. W. Blöte, J. L. Cardy and M. P. Nightingale. Conformal invariance, the central charge, and universal finite-size amplitudes at criticality. Physical Review Letters 56, 742–745 (1986).
[32]
P. Calabrese and J. Cardy. Entanglement entropy and quantum field theory. Journal of Statistical Mechanics: Theory and Experiment 2004, P06002 (2004).
[35]
J. L. Cardy. Operator content of two-dimensional conformally invariant theories. Nuclear Physics B 270, 186–204 (1986).
[85]
S. Eggert, I. Affleck and M. Takahashi. Susceptibility of the spin 1/2 Heisenberg antiferromagnetic chain. Physical Review Letters 73, 332–335 (1994).
[86]
F. D. Haldane. General Relation of Correlation Exponents and Spectral Properties of One-Dimensional Fermi Systems: Application to the Anisotropic $S=1/2$ Heisenberg Chain. Physical Review Letters 45, 1358–1362 (1980).
[87]
L. Hulthén. Über das Austauschproblem eines Kristalles. Arkiv för Matematik, Astronomi och Fysik 26A, 1–106 (1938).
[88]
A. Luther and I. Peschel. Calculation of critical exponents in two dimensions from quantum field theory in one dimension. Physical Review B 12, 3908–3917 (1975).
[89]
G. Müller, H. Thomas, H. Beck and J. C. Bonner. Quantum spin dynamics of the antiferromagnetic linear chain in zero and nonzero magnetic field. Physical Review B 24, 1429–1467 (1981).
[90]
J. des Cloizeaux and J. J. Pearson. Spin-Wave Spectrum of the Antiferromagnetic Linear Chain. Physical Review 128, 2131–2135 (1962).

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