š¢ Heisenberg1D/ThermalEntropy/OBC
Generated by docs/atlas/generate.jl ā 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 ā a hub can read green while its @test is red between regenerations. @sweep = a graceful regime-resolution gap, not card omission.
src claim
- method
dense_ed, statusexact, reliabilityhigh
Corroboration
| regime | mechanism | independence | refs | file |
|---|---|---|---|---|
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | limiting_case | š” asserted | Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermal_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
@su2 | ed_finite_size | š¢ structural | ED black-box: S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_heisenberg1d_obc_thermo_ED_batch.jl |
Test calls
The exact verify(...) call the harness executed for this hub (reconstructed from the test AST):
verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :limiting_case, independent = if iseven(4) 0.0 else log(2.0) / 4 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 0.5 = 0.5, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 0.5 = 0.5, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :limiting_case, independent = if iseven(6) 0.0 else log(2.0) / 6 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 0.5 = 0.5, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 0.5 = 0.5, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :limiting_case, independent = if iseven(8) 0.0 else log(2.0) / 8 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 0.5 = 0.5, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 0.5 = 0.5, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :limiting_case, independent = if iseven(4) 0.0 else log(2.0) / 4 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 1.0 = 1.0, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 1.0 = 1.0, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :limiting_case, independent = if iseven(6) 0.0 else log(2.0) / 6 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 1.0 = 1.0, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 1.0 = 1.0, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :limiting_case, independent = if iseven(8) 0.0 else log(2.0) / 8 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 1.0 = 1.0, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 1.0 = 1.0, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :limiting_case, independent = if iseven(4) 0.0 else log(2.0) / 4 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 2.0 = 2.0, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 2.0 = 2.0, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :limiting_case, independent = if iseven(6) 0.0 else log(2.0) / 6 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 2.0 = 2.0, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 2.0 = 2.0, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :limiting_case, independent = if iseven(8) 0.0 else log(2.0) / 8 end, agree_within = 1.0e-9, refs = ["Heisenberg1D OBC T ā 0: singlet GS for even N ā s = 0; doublet GS for odd N ā s = log(2)/N"], fetch_kw = (; 2.0 = 2.0, beta = 1.0e6))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :limiting_case, independent = log(2), agree_within = 1.0e-5, refs = ["Heisenberg1D OBC T ā ā: free paramagnet ā s = log 2 per spin"], fetch_kw = (; 2.0 = 2.0, beta = 0.001))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 1.0 = 1.0, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(6); route = :ed_finite_size, independent = ed_S, at = ["N=$(6)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 10.0 = 10.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(0.5)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 0.5 = 0.5))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(2.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 2.0 = 2.0))verify(Heisenberg1D(), ThermalEntropy(), OBC(8); route = :ed_finite_size, independent = ed_S, at = ["N=$(8)", "Ī²=$(10.0)"], agree_within = 1.0e-9, refs = ["ED black-box: S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0, 10.0 = 10.0))Assurance (provisional)
- level: corroborated-at-p š¢
- cards: 45 Ā· model ED-feasible
- RES not wired ā measured residuals / confidence are not shown yet.
ā Model: Heisenberg1D Ā· Quantity: ThermalEntropy Ā· Atlas index