ShastrySutherland — model index

Spin-½ Shastry–Sutherland model on the Shastry–Sutherland lattice (corner-sharing-orthogonal-dimer geometry; realised in SrCu₂(BO₃)₂):

H = J Σ_{⟨i,j⟩} Sᵢ · Sⱼ + J' Σ_{⟨⟨i,j⟩⟩_d} Sᵢ · Sⱼ.
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 ShastrySutherland. 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-p0
🔵 coherent0
⚪ cited-only0
🟠 uncorroborated-but-feasible1
total claimed hubs1

Methods (from @register, derived): exact_dimer

Quantity × BC matrix

QuantityInfinite
Energy🟠 hub

References

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

[72]
A. Koga and N. Kawakami. Quantum Phase Transitions in the Shastry-Sutherland Model for SrCu$_2$(BO$_3$)$_2$. Physical Review Letters 84, 4461–4464 (2000).
[73]
B. Sriram Shastry and B. Sutherland. Exact ground state of a quantum mechanical antiferromagnet. Physica B+C 108, 1069–1070 (1981).

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