🔵 S1Heisenberg1D/MagnetizationY/OBC
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.
An independent card exists and the value satisfies an internal invariant; no external value re-derives it yet.
src claim
- method
dense_ed, statusexact, reliabilityhigh
Corroboration
| regime | mechanism | independence | refs | file |
|---|---|---|---|---|
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
@haldane | limiting_case | 🟡 asserted | SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_mag_batch.jl |
Test calls
The exact verify(...) call the harness executed for this hub (reconstructed from the test AST):
verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(3); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(3); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(5); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(5); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 0.5 = 0.5), MagnetizationY(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(3); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(3); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(5); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(5); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 1.0 = 1.0), MagnetizationY(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(3); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(3); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(5); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(5); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 1.0))verify(S1Heisenberg1D(; 2.0 = 2.0), MagnetizationY(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of S=1 Heisenberg: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble"], fetch_kw = (; beta = 10.0))Assurance (provisional)
- level: coherent 🔵
- cards: 24 · model ED-feasible
- RES not wired — measured residuals / confidence are not shown yet.
← Model: S1Heisenberg1D · Quantity: MagnetizationY · Atlas index