GitHub

🔵 Heisenberg1D/MagnetizationZ/OBC

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.

Assurance level: coherent

An independent card exists and the value satisfies an internal invariant; no external value re-derives it yet.

src claim

  • method dense_ed, status exact, reliability high

Corroboration

regimemechanismindependencerefsfile
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl
@su2limiting_case🟡 assertedSU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, βtest/models/quantum/Heisenberg/test_heisenberg1d_obc_mag_batch.jl

Test calls

The exact verify(...) call the harness executed for this hub (reconstructed from the test AST):

verify(Heisenberg1D(), MagnetizationZ(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 0.5 = 0.5, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 0.5 = 0.5, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 0.5 = 0.5, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 0.5 = 0.5, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(8); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 0.5 = 0.5, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(8); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 0.5 = 0.5, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 1.0 = 1.0, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 1.0 = 1.0, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 1.0 = 1.0, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 1.0 = 1.0, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(8); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 1.0 = 1.0, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(8); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 1.0 = 1.0, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 2.0 = 2.0, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(4); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 2.0 = 2.0, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 2.0 = 2.0, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(6); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 2.0 = 2.0, beta = 10.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(8); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 2.0 = 2.0, beta = 1.0))
verify(Heisenberg1D(), MagnetizationZ(), OBC(8); route = :limiting_case, independent = 0.0, agree_within = 1.0e-10, refs = ["SU(2) symmetry of the Heisenberg Hamiltonian: <S^α>_β = 0 for α ∈ {x,y,z} in the unbroken thermal ensemble, exact for any J, N, β"], fetch_kw = (; 2.0 = 2.0, beta = 10.0))

Assurance (provisional)

  • level: coherent 🔵
  • cards: 18 · model ED-feasible
  • RES not wired — measured residuals / confidence are not shown yet.

← Model: Heisenberg1D · Quantity: MagnetizationZ · Atlas index