{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:XCKSSDVKHME5OUVHPOHVRB3IOR","short_pith_number":"pith:XCKSSDVK","schema_version":"1.0","canonical_sha256":"b895290eaa3b09d752a77b8f58876874623bfab230581bc0c4d299eb9d4c7ca1","source":{"kind":"arxiv","id":"1403.1406","version":2},"attestation_state":"computed","paper":{"title":"Baxter-Wu model in a transverse magnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Fabien Alet, Kai Phillip Schmidt, Saeed S. Jahromi, Sylvain Capponi","submitted_at":"2014-03-06T11:11:00Z","abstract_excerpt":"We investigate the low-energy properties as well as quantum and thermal phase transitions of the Baxter-Wu model in a transverse magnetic field. Our study relies on stochastic series expansion quantum Monte Carlo and on series expansions about the low- and high-field limits at zero temperature using the quantum finite-lattice method on the triangular lattice. The phase boundary consists of a second-order critical line in the 4-state Potts model universality class starting from the pure Baxter-Wu limit meeting a first-order line connected to the zero-temperature transition point ($h\\approx2.4$,"},"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":"1403.1406","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2014-03-06T11:11:00Z","cross_cats_sorted":["cond-mat.stat-mech"],"title_canon_sha256":"6af277468ce760618e2c841b096061dd886171c8b2068deb37a068eb095f7c4a","abstract_canon_sha256":"f2e84e9916ad7dfd26ad2284e99cb8c1ec468ddba4b7fec0f0383e8e135d1c0f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:48:09.530284Z","signature_b64":"KUVrzxbnnRBKWGEISghPfKQs5AC5oa8rVjKOgLYmKKaABWgQ32P8s8Y7aLOx8rwheSSn6UFbZ1gV59XvqCdMAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b895290eaa3b09d752a77b8f58876874623bfab230581bc0c4d299eb9d4c7ca1","last_reissued_at":"2026-05-18T02:48:09.529908Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:48:09.529908Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Baxter-Wu model in a transverse magnetic field","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.stat-mech"],"primary_cat":"cond-mat.str-el","authors_text":"Fabien Alet, Kai Phillip Schmidt, Saeed S. Jahromi, Sylvain Capponi","submitted_at":"2014-03-06T11:11:00Z","abstract_excerpt":"We investigate the low-energy properties as well as quantum and thermal phase transitions of the Baxter-Wu model in a transverse magnetic field. Our study relies on stochastic series expansion quantum Monte Carlo and on series expansions about the low- and high-field limits at zero temperature using the quantum finite-lattice method on the triangular lattice. The phase boundary consists of a second-order critical line in the 4-state Potts model universality class starting from the pure Baxter-Wu limit meeting a first-order line connected to the zero-temperature transition point ($h\\approx2.4$,"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.1406","kind":"arxiv","version":2},"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":"1403.1406","created_at":"2026-05-18T02:48:09.529963+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.1406v2","created_at":"2026-05-18T02:48:09.529963+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.1406","created_at":"2026-05-18T02:48:09.529963+00:00"},{"alias_kind":"pith_short_12","alias_value":"XCKSSDVKHME5","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_16","alias_value":"XCKSSDVKHME5OUVH","created_at":"2026-05-18T12:28:57.508820+00:00"},{"alias_kind":"pith_short_8","alias_value":"XCKSSDVK","created_at":"2026-05-18T12:28:57.508820+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/XCKSSDVKHME5OUVHPOHVRB3IOR","json":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR.json","graph_json":"https://pith.science/api/pith-number/XCKSSDVKHME5OUVHPOHVRB3IOR/graph.json","events_json":"https://pith.science/api/pith-number/XCKSSDVKHME5OUVHPOHVRB3IOR/events.json","paper":"https://pith.science/paper/XCKSSDVK"},"agent_actions":{"view_html":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR","download_json":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR.json","view_paper":"https://pith.science/paper/XCKSSDVK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.1406&json=true","fetch_graph":"https://pith.science/api/pith-number/XCKSSDVKHME5OUVHPOHVRB3IOR/graph.json","fetch_events":"https://pith.science/api/pith-number/XCKSSDVKHME5OUVHPOHVRB3IOR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR/action/storage_attestation","attest_author":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR/action/author_attestation","sign_citation":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR/action/citation_signature","submit_replication":"https://pith.science/pith/XCKSSDVKHME5OUVHPOHVRB3IOR/action/replication_record"}},"created_at":"2026-05-18T02:48:09.529963+00:00","updated_at":"2026-05-18T02:48:09.529963+00:00"}