{ "model": "ShastrySutherland", "lattice": "square", "n_sites": 400, "boundary": "O", "params": { "J": 0.8, "Jd": 1 }, "cluster": "20 x 20 square lattice with orthogonal dimers, open boundaries, setup B of arXiv:2309.10955 App. S-2 (the corner sites carry no dimer bond)", "instance_id": "ShastrySutherland/square_400_O_J0.8_Jd1", "rows": [ { "energy": -707.3664, "sigma": 0.0128, "energy_variance": null, "dof": 400, "einf": 0, "v_score": null, "method": "PEPS", "ansatz": null, "method_detail": "finite", "method_as_published": "finite PEPS, D = 4", "family": "tensor network", "bound_type": "variational", "bound_type_reason": "variational ansatz at a stated size; energy is an upper bound (assigned during source reading)", "reference": "Liu, Zhang, Wang, Gong, Chen & Gu, Quantum Criticality with Emergent Symmetry in the Extended Shastry-Sutherland Model, Phys. Rev. Lett. 133, 026502 (2024), doi:10.1103/PhysRevLett.133.026502, arXiv:2309.10955", "peer_reviewed": true, "source": "sweep-allresults-2026-10-20", "provenance": "primary", "verified": { "checked_on": "2026-10-20", "method": "source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)", "reported_as": "-0.442104(8)", "note": "Table III, D = 4; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.", "secondary_of": null, "second_read": { "checked_on": "2026-10-24", "scope": "value", "method": "arXiv:2309.10955v2 PDF (SM Table III), pypdf layout mode; v1 Table III identical; PRL 133, 026502 accepted manuscript (CHORUS) for the main text; APS SM not reachable (HTTP 401)", "location": "SM Table III, row D = 4, column E", "reported_as": "-0.442104(8) (S.S units, per site of the 20 x 20 open lattice (setup B), J1/J2 = 0.8 with J2 = 1)", "conversion": "-0.442104 x 1600 = -707.3664; sigma 8e-06 x 1600 = 0.0128", "note": "Own computation; Eq. (1) is the instance's H (J = J1 = 0.8 on square bonds, Jd = J2 = 1 on dimers, S.S, no shift); open 20 x 20, setup B (App. S-2); fixed-D finite PEPS energy sampled by MC, variational, sampled; sigma = printed MC error x 1600. Whole-lattice per-site reading supported by the size of the open-edge loss (1.5% above the periodic 10 x 10 value). Journal main text agrees with arXiv; the journal SM was not reachable (APS 401), arXiv v2 (2024-05-29) post-dates the accepted manuscript (2024-05-21). No other batch's row on the instance.", "source_entry": "famP6-shastrysutherland-j1j2-heisenberg#0 (qmbl-verify 2026-10-23)" } }, "compute": { "parameters": null, "gpu_hours": null, "device": null, "n_devices": null, "samples": null, "wall_clock": null, "cpu_core_hours": null, "bond_dimension": 4, "iterations": null, "reported_as": "method string: \"finite PEPS, D = 4\"", "source": "the row's published method string (scripts/method_names.mjs, 2026-09-17)", "scope": "row", "confidence": "high", "note": "Only the numbers the method string states; nothing else about this run's cost is recorded." } }, { "energy": -708.5776, "sigma": 0.0144, "energy_variance": null, "dof": 400, "einf": 0, "v_score": null, "method": "PEPS", "ansatz": null, "method_detail": "finite", "method_as_published": "finite PEPS, D = 6", "family": "tensor network", "bound_type": "variational", "bound_type_reason": "variational ansatz at a stated size; energy is an upper bound (assigned during source reading)", "reference": "Liu, Zhang, Wang, Gong, Chen & Gu, Quantum Criticality with Emergent Symmetry in the Extended Shastry-Sutherland Model, Phys. Rev. Lett. 133, 026502 (2024), doi:10.1103/PhysRevLett.133.026502, arXiv:2309.10955", "peer_reviewed": true, "source": "sweep-allresults-2026-10-20", "provenance": "primary", "verified": { "checked_on": "2026-10-20", "method": "source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)", "reported_as": "-0.442861(9)", "note": "Table III, D = 6; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.", "secondary_of": null, "second_read": { "checked_on": "2026-10-24", "scope": "value", "method": "arXiv:2309.10955v2 PDF (SM Table III), pypdf layout mode; v1 Table III identical; PRL 133, 026502 accepted manuscript (CHORUS) for the main text; APS SM not reachable (HTTP 401)", "location": "SM Table III, row D = 6, column E", "reported_as": "-0.442861(9) (S.S units, per site of the 20 x 20 open lattice (setup B), J1/J2 = 0.8 with J2 = 1)", "conversion": "-0.442861 x 1600 = -708.5776; sigma 9e-06 x 1600 = 0.0144", "note": "Own computation; Eq. (1) is the instance's H (J = J1 = 0.8 on square bonds, Jd = J2 = 1 on dimers, S.S, no shift); open 20 x 20, setup B (App. S-2); fixed-D finite PEPS energy sampled by MC, variational, sampled; sigma = printed MC error x 1600. Whole-lattice per-site reading supported by the size of the open-edge loss (1.5% above the periodic 10 x 10 value). Journal main text agrees with arXiv; the journal SM was not reachable (APS 401), arXiv v2 (2024-05-29) post-dates the accepted manuscript (2024-05-21). No other batch's row on the instance.", "source_entry": "famP6-shastrysutherland-j1j2-heisenberg#1 (qmbl-verify 2026-10-23)" } }, "compute": { "parameters": null, "gpu_hours": null, "device": null, "n_devices": null, "samples": null, "wall_clock": null, "cpu_core_hours": null, "bond_dimension": 6, "iterations": null, "reported_as": "method string: \"finite PEPS, D = 6\"", "source": "the row's published method string (scripts/method_names.mjs, 2026-09-17)", "scope": "row", "confidence": "high", "note": "Only the numbers the method string states; nothing else about this run's cost is recorded." } }, { "energy": -708.672, "sigma": 0.0032, "energy_variance": null, "dof": 400, "einf": 0, "v_score": null, "method": "PEPS", "ansatz": null, "method_detail": "finite", "method_as_published": "finite PEPS, D = 8", "family": "tensor network", "bound_type": "variational", "bound_type_reason": "variational ansatz at a stated size; energy is an upper bound (assigned during source reading)", "reference": "Liu, Zhang, Wang, Gong, Chen & Gu, Quantum Criticality with Emergent Symmetry in the Extended Shastry-Sutherland Model, Phys. Rev. Lett. 133, 026502 (2024), doi:10.1103/PhysRevLett.133.026502, arXiv:2309.10955", "peer_reviewed": true, "source": "sweep-allresults-2026-10-20", "provenance": "primary", "verified": { "checked_on": "2026-10-20", "method": "source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)", "reported_as": "-0.442920(2)", "note": "Table III, D = 8; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.", "secondary_of": null, "second_read": { "checked_on": "2026-10-24", "scope": "value", "method": "arXiv:2309.10955v2 PDF (SM Table III), pypdf layout mode; v1 Table III identical; PRL 133, 026502 accepted manuscript (CHORUS) for the main text; APS SM not reachable (HTTP 401)", "location": "SM Table III, row D = 8, column E", "reported_as": "-0.442920(2) (S.S units, per site of the 20 x 20 open lattice (setup B), J1/J2 = 0.8 with J2 = 1)", "conversion": "-0.44292 x 1600 = -708.672; sigma 2e-06 x 1600 = 0.0032", "note": "Own computation; Eq. (1) is the instance's H (J = J1 = 0.8 on square bonds, Jd = J2 = 1 on dimers, S.S, no shift); open 20 x 20, setup B (App. S-2); fixed-D finite PEPS energy sampled by MC, variational, sampled; sigma = printed MC error x 1600. Whole-lattice per-site reading supported by the size of the open-edge loss (1.5% above the periodic 10 x 10 value). Journal main text agrees with arXiv; the journal SM was not reachable (APS 401), arXiv v2 (2024-05-29) post-dates the accepted manuscript (2024-05-21). No other batch's row on the instance.", "source_entry": "famP6-shastrysutherland-j1j2-heisenberg#2 (qmbl-verify 2026-10-23)" } }, "compute": { "parameters": null, "gpu_hours": null, "device": null, "n_devices": null, "samples": null, "wall_clock": null, "cpu_core_hours": null, "bond_dimension": 8, "iterations": null, "reported_as": "method string: \"finite PEPS, D = 8\"", "source": "the row's published method string (scripts/method_names.mjs, 2026-09-17)", "scope": "row", "confidence": "high", "note": "Only the numbers the method string states; nothing else about this run's cost is recorded." } }, { "energy": -708.6848, "sigma": 0.0048, "energy_variance": null, "dof": 400, "einf": 0, "v_score": null, "method": "PEPS", "ansatz": null, "method_detail": "finite", "method_as_published": "finite PEPS, D = 10", "family": "tensor network", "bound_type": "variational", "bound_type_reason": "variational ansatz at a stated size; energy is an upper bound (assigned during source reading)", "reference": "Liu, Zhang, Wang, Gong, Chen & Gu, Quantum Criticality with Emergent Symmetry in the Extended Shastry-Sutherland Model, Phys. Rev. Lett. 133, 026502 (2024), doi:10.1103/PhysRevLett.133.026502, arXiv:2309.10955", "peer_reviewed": true, "source": "sweep-allresults-2026-10-20", "provenance": "primary", "verified": { "checked_on": "2026-10-20", "method": "source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)", "reported_as": "-0.442928(3)", "note": "Table III, D = 10; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.", "secondary_of": null, "second_read": { "checked_on": "2026-10-24", "scope": "value", "method": "arXiv:2309.10955v2 PDF (SM Table III), pypdf layout mode; v1 Table III identical; PRL 133, 026502 accepted manuscript (CHORUS) for the main text; APS SM not reachable (HTTP 401)", "location": "SM Table III, row D = 10, column E", "reported_as": "-0.442928(3) (S.S units, per site of the 20 x 20 open lattice (setup B), J1/J2 = 0.8 with J2 = 1)", "conversion": "-0.442928 x 1600 = -708.6848; sigma 3e-06 x 1600 = 0.0048", "note": "Own computation; Eq. (1) is the instance's H (J = J1 = 0.8 on square bonds, Jd = J2 = 1 on dimers, S.S, no shift); open 20 x 20, setup B (App. S-2); fixed-D finite PEPS energy sampled by MC, variational, sampled; sigma = printed MC error x 1600. Whole-lattice per-site reading supported by the size of the open-edge loss (1.5% above the periodic 10 x 10 value). Journal main text agrees with arXiv; the journal SM was not reachable (APS 401), arXiv v2 (2024-05-29) post-dates the accepted manuscript (2024-05-21). No other batch's row on the instance. Record row: D = 10 sits 8e-6 per site (2.2 combined sigma) below D = 8; the paper calls D = 8 converged.", "source_entry": "famP6-shastrysutherland-j1j2-heisenberg#3 (qmbl-verify 2026-10-23)" } }, "compute": { "parameters": null, "gpu_hours": null, "device": null, "n_devices": null, "samples": null, "wall_clock": null, "cpu_core_hours": null, "bond_dimension": 10, "iterations": null, "reported_as": "method string: \"finite PEPS, D = 10\"", "source": "the row's published method string (scripts/method_names.mjs, 2026-09-17)", "scope": "row", "confidence": "high", "note": "Only the numbers the method string states; nothing else about this run's cost is recorded." } } ], "url": "https://qmbl.org/i/ShastrySutherland/square_400_O_J0.8_Jd1/", "per_site_divisor": 1600, "per_site_label": "E/N (S.S)", "best": { "exact": null, "variational": { "energy": -708.6848, "sigma": 0.0048, "method": "PEPS", "ansatz": null, "method_detail": "finite", "reference": "Liu, Zhang, Wang, Gong, Chen & Gu, Quantum Criticality with Emergent Symmetry in the Extended Shastry-Sutherland Model, Phys. Rev. Lett. 133, 026502 (2024), doi:10.1103/PhysRevLett.133.026502, arXiv:2309.10955", "bound_type": "variational", "energy_per_site": -0.442928 }, "projected": null, "extrapolated": null, "approximate": null, "below_exact": [] }, "no_best_reason": null, "record": { "energy": -708.6848, "sigma": 0.0048, "method": "PEPS", "ansatz": null, "method_detail": "finite", "reference": "Liu, Zhang, Wang, Gong, Chen & Gu, Quantum Criticality with Emergent Symmetry in the Extended Shastry-Sutherland Model, Phys. Rev. Lett. 133, 026502 (2024), doi:10.1103/PhysRevLett.133.026502, arXiv:2309.10955", "bound_type": "variational", "energy_per_site": -0.442928 }, "no_record_reason": null }