{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:ST5YVAHVFMRXFGUAFJI42KVXLU","short_pith_number":"pith:ST5YVAHV","schema_version":"1.0","canonical_sha256":"94fb8a80f52b23729a802a51cd2ab75d2528fe11b2c60ff445ce0393e9ddb089","source":{"kind":"arxiv","id":"1410.0822","version":1},"attestation_state":"computed","paper":{"title":"Reentrance of Berezinskii-Kosterlitz-Thouless-like transitions in three-state Potts antiferromagnetic thin film","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Chengxiang Ding, Wenan Guo, Youjin Deng","submitted_at":"2014-10-03T11:22:21Z","abstract_excerpt":"Using Monte Carlo simulations and finite-size scaling, we study three-state Potts antiferromagnet on layered square lattice with two and four layers $L_z=2$ and $4$. As temperature decreases, the system develops quasi-long-range order via a Berezinskii-Kosterlitz-Thouless transition at finite temperature $T_{c1}$. For $L_z=4$, as temperature is further lowered, a long-range order breaking the $Z_6$ symmetry develops at a second transition at $T_{c2} < T_{c1}$. The transition at $T_{c2}$ is also Berezinskii-Kosterlitz-Thouless-like, but has magnetic critical exponent $\\eta=1/9$ instead of the c"},"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":"1410.0822","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.stat-mech","submitted_at":"2014-10-03T11:22:21Z","cross_cats_sorted":[],"title_canon_sha256":"053d1cde2130a549afbc4670328e447a54b5d438e24625edbcf0cd6017dae17d","abstract_canon_sha256":"26ea89606d0f10762956775b6fed7e68c3a18cfa3931edc90ed50be31e3146f7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:41:52.867797Z","signature_b64":"dZmT3oOfSRpHczg/z67k6Ny8Ww+ZMU4gorMWCjdc8wy1Rhn4UeC427yNGhqOD4Nrz5RsJOkEyqAn3ULYNlR0Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"94fb8a80f52b23729a802a51cd2ab75d2528fe11b2c60ff445ce0393e9ddb089","last_reissued_at":"2026-05-18T01:41:52.867287Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:41:52.867287Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Reentrance of Berezinskii-Kosterlitz-Thouless-like transitions in three-state Potts antiferromagnetic thin film","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.stat-mech","authors_text":"Chengxiang Ding, Wenan Guo, Youjin Deng","submitted_at":"2014-10-03T11:22:21Z","abstract_excerpt":"Using Monte Carlo simulations and finite-size scaling, we study three-state Potts antiferromagnet on layered square lattice with two and four layers $L_z=2$ and $4$. As temperature decreases, the system develops quasi-long-range order via a Berezinskii-Kosterlitz-Thouless transition at finite temperature $T_{c1}$. For $L_z=4$, as temperature is further lowered, a long-range order breaking the $Z_6$ symmetry develops at a second transition at $T_{c2} < T_{c1}$. The transition at $T_{c2}$ is also Berezinskii-Kosterlitz-Thouless-like, but has magnetic critical exponent $\\eta=1/9$ instead of the c"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.0822","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":"1410.0822","created_at":"2026-05-18T01:41:52.867373+00:00"},{"alias_kind":"arxiv_version","alias_value":"1410.0822v1","created_at":"2026-05-18T01:41:52.867373+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.0822","created_at":"2026-05-18T01:41:52.867373+00:00"},{"alias_kind":"pith_short_12","alias_value":"ST5YVAHVFMRX","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"ST5YVAHVFMRXFGUA","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"ST5YVAHV","created_at":"2026-05-18T12:28:49.207871+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/ST5YVAHVFMRXFGUAFJI42KVXLU","json":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU.json","graph_json":"https://pith.science/api/pith-number/ST5YVAHVFMRXFGUAFJI42KVXLU/graph.json","events_json":"https://pith.science/api/pith-number/ST5YVAHVFMRXFGUAFJI42KVXLU/events.json","paper":"https://pith.science/paper/ST5YVAHV"},"agent_actions":{"view_html":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU","download_json":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU.json","view_paper":"https://pith.science/paper/ST5YVAHV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1410.0822&json=true","fetch_graph":"https://pith.science/api/pith-number/ST5YVAHVFMRXFGUAFJI42KVXLU/graph.json","fetch_events":"https://pith.science/api/pith-number/ST5YVAHVFMRXFGUAFJI42KVXLU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU/action/storage_attestation","attest_author":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU/action/author_attestation","sign_citation":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU/action/citation_signature","submit_replication":"https://pith.science/pith/ST5YVAHVFMRXFGUAFJI42KVXLU/action/replication_record"}},"created_at":"2026-05-18T01:41:52.867373+00:00","updated_at":"2026-05-18T01:41:52.867373+00:00"}