š¢ S1Heisenberg1D/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 |
|---|---|---|---|---|
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1H OBC at T ā 0: edge-multiplet residue spersite = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | limiting_case | š” asserted | S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermal_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_batch.jl |
@haldane | ed_finite_size | š¢ structural | ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum | test/models/quantum/Heisenberg/test_s1heisenberg1d_obc_thermo_ED_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), ThermalEntropy(), OBC(3); route = :limiting_case, independent = if iseven(3) 0.0 else log(3) / 3 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(3); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(4); route = :limiting_case, independent = if iseven(4) 0.0 else log(3) / 4 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(4); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(5); route = :limiting_case, independent = if iseven(5) 0.0 else log(3) / 5 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(5); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(3); route = :limiting_case, independent = if iseven(3) 0.0 else log(3) / 3 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(3); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(4); route = :limiting_case, independent = if iseven(4) 0.0 else log(3) / 4 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(4); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(5); route = :limiting_case, independent = if iseven(5) 0.0 else log(3) / 5 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(5); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(3); route = :limiting_case, independent = if iseven(3) 0.0 else log(3) / 3 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(3); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(4); route = :limiting_case, independent = if iseven(4) 0.0 else log(3) / 4 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(4); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(5); route = :limiting_case, independent = if iseven(5) 0.0 else log(3) / 5 end, agree_within = 1.0e-9, refs = ["S1H OBC at T ā 0: edge-multiplet residue s_per_site = iseven(N) ? 0 : log(3)/N for finite N (triplet GS for odd N, singlet for even N); Haldane-gap unique GS recovered only in N ā ā"], fetch_kw = (; beta = 1.0e6))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(5); route = :limiting_case, independent = log(3), agree_within = 1.0e-5, refs = ["S1Heisenberg1D OBC T ā ā: spin-1 paramagnet ā s = log 3 per spin"], fetch_kw = (; beta = 0.001))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 0.5 = 0.5), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 1.0 = 1.0), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(3); route = :ed_finite_size, independent = ed_S, at = ["N=$(3)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(4); route = :ed_finite_size, independent = ed_S, at = ["N=$(4)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 0.5 = 0.5))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 2.0 = 2.0))verify(S1Heisenberg1D(; 2.0 = 2.0), ThermalEntropy(), OBC(5); route = :ed_finite_size, independent = ed_S, at = ["N=$(5)"], agree_within = 1.0e-9, refs = ["ED black-box (spin-1): S = Ī²Ā·(E - F) from full spectrum"], fetch_kw = (; 5.0 = 5.0))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: S1Heisenberg1D Ā· Quantity: ThermalEntropy Ā· Atlas index