{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:2WNOPJGMSEX65WGURJIWFUIAY5","short_pith_number":"pith:2WNOPJGM","schema_version":"1.0","canonical_sha256":"d59ae7a4cc912feed8d48a5162d100c77ad39ce5a8f75b47ca3ed351e36639fc","source":{"kind":"arxiv","id":"1901.10643","version":1},"attestation_state":"computed","paper":{"title":"Finite size scaling for a first order transition where a continuous symmetry is broken: The spin-flop transition in the 3D XXZ Heisenberg antiferromagnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"physics.comp-ph","authors_text":"D. P. Landau, Jiahao Xu, K. Binder, Shan-Ho Tsai","submitted_at":"2019-01-30T02:12:31Z","abstract_excerpt":"Finite size scaling for a first order phase transition where a continuous symmetry is broken is developed using an approximation of Gaussian probability distributions with a phenomenological \"degeneracy\" factor included. Predictions are compared with data from Monte Carlo simulations of the three-dimensional, XXZ Heisenberg antiferromagnet in a field in order to study the finite size behavior on a $L \\times L \\times L$ simple cubic lattice for the first order \"spin-flop\" transition between the Ising-like antiferromagnetic state and the canted, XY-like state. Our theory predicts that for large "},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1901.10643","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2019-01-30T02:12:31Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"ab849495971ce0c77c5b1d2c5c606a1ff615c4f993119c807204f43fde37efd3","abstract_canon_sha256":"633e2df0cc6688258825f5eb71847851ef9ed64de40cacbc1d24fdb898d0670c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:21.612547Z","signature_b64":"SCh3+vUgth5qvZwvJceMhyhHHFpZWX/EWQGWXdbRFqZJ5AN9g0jaSoxIO1VsZRif6xh4c7SoaEuBeM9vOPDRDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d59ae7a4cc912feed8d48a5162d100c77ad39ce5a8f75b47ca3ed351e36639fc","last_reissued_at":"2026-05-17T23:50:21.611910Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:21.611910Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Finite size scaling for a first order transition where a continuous symmetry is broken: The spin-flop transition in the 3D XXZ Heisenberg antiferromagnet","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"physics.comp-ph","authors_text":"D. P. Landau, Jiahao Xu, K. Binder, Shan-Ho Tsai","submitted_at":"2019-01-30T02:12:31Z","abstract_excerpt":"Finite size scaling for a first order phase transition where a continuous symmetry is broken is developed using an approximation of Gaussian probability distributions with a phenomenological \"degeneracy\" factor included. Predictions are compared with data from Monte Carlo simulations of the three-dimensional, XXZ Heisenberg antiferromagnet in a field in order to study the finite size behavior on a $L \\times L \\times L$ simple cubic lattice for the first order \"spin-flop\" transition between the Ising-like antiferromagnetic state and the canted, XY-like state. Our theory predicts that for large "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.10643","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"1901.10643","created_at":"2026-05-17T23:50:21.611998+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.10643v1","created_at":"2026-05-17T23:50:21.611998+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.10643","created_at":"2026-05-17T23:50:21.611998+00:00"},{"alias_kind":"pith_short_12","alias_value":"2WNOPJGMSEX6","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_16","alias_value":"2WNOPJGMSEX65WGU","created_at":"2026-05-18T12:33:07.085635+00:00"},{"alias_kind":"pith_short_8","alias_value":"2WNOPJGM","created_at":"2026-05-18T12:33:07.085635+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5","json":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5.json","graph_json":"https://pith.science/api/pith-number/2WNOPJGMSEX65WGURJIWFUIAY5/graph.json","events_json":"https://pith.science/api/pith-number/2WNOPJGMSEX65WGURJIWFUIAY5/events.json","paper":"https://pith.science/paper/2WNOPJGM"},"agent_actions":{"view_html":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5","download_json":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5.json","view_paper":"https://pith.science/paper/2WNOPJGM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.10643&json=true","fetch_graph":"https://pith.science/api/pith-number/2WNOPJGMSEX65WGURJIWFUIAY5/graph.json","fetch_events":"https://pith.science/api/pith-number/2WNOPJGMSEX65WGURJIWFUIAY5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5/action/storage_attestation","attest_author":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5/action/author_attestation","sign_citation":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5/action/citation_signature","submit_replication":"https://pith.science/pith/2WNOPJGMSEX65WGURJIWFUIAY5/action/replication_record"}},"created_at":"2026-05-17T23:50:21.611998+00:00","updated_at":"2026-05-17T23:50:21.611998+00:00"}