{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:ZY2GV3PQBJI6VNMWBX5BZNJABW","short_pith_number":"pith:ZY2GV3PQ","schema_version":"1.0","canonical_sha256":"ce346aedf00a51eab5960dfa1cb5200d996443869d9628994309af9576b9dad1","source":{"kind":"arxiv","id":"1704.01318","version":1},"attestation_state":"computed","paper":{"title":"Effect of long-and short-range interactions on the thermodynamics of dipolar spin ice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"physics.comp-ph","authors_text":"Aleksandr Makarov, Konstantin Nefedev, Yuriy Shevchenko","submitted_at":"2017-04-05T09:19:58Z","abstract_excerpt":"The thermodynamic properties of dipolar spin ice on square, honeycomb and shakti lattices in the long-range and short-range dipole interaction models are studied. Exact solutions for the density of states, temperature dependencies of heat capacity, and entropy are obtained for these lattices with a finite number of point dipoles by means of complete enumeration. The magnetic susceptibility and average size of the largest low-energy cluster are calculated for square spin ice by means of Wang-Landau and Metropolis methods. We show that the long-range interaction leads to a blurring of the energy"},"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":"1704.01318","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.comp-ph","submitted_at":"2017-04-05T09:19:58Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"cc37dd2d3f679e9f68f8df2e260ee716c96e64052d7a4d1a0095bee27369e7e4","abstract_canon_sha256":"82e002b75ca161629ed4c60d2bbaeea81879bd9b986ab782eee523387dcf2e45"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:46:58.473783Z","signature_b64":"/bT04IHIBLze2IXfDOSlo089uqwXtZi3hLI3lR6Suk5WRxFBQIvvz2Nj+rONTVBEVhEIwOFK7aHpQPvPjJShDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ce346aedf00a51eab5960dfa1cb5200d996443869d9628994309af9576b9dad1","last_reissued_at":"2026-05-18T00:46:58.473328Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:46:58.473328Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effect of long-and short-range interactions on the thermodynamics of dipolar spin ice","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"physics.comp-ph","authors_text":"Aleksandr Makarov, Konstantin Nefedev, Yuriy Shevchenko","submitted_at":"2017-04-05T09:19:58Z","abstract_excerpt":"The thermodynamic properties of dipolar spin ice on square, honeycomb and shakti lattices in the long-range and short-range dipole interaction models are studied. Exact solutions for the density of states, temperature dependencies of heat capacity, and entropy are obtained for these lattices with a finite number of point dipoles by means of complete enumeration. The magnetic susceptibility and average size of the largest low-energy cluster are calculated for square spin ice by means of Wang-Landau and Metropolis methods. We show that the long-range interaction leads to a blurring of the energy"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1704.01318","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":"1704.01318","created_at":"2026-05-18T00:46:58.473397+00:00"},{"alias_kind":"arxiv_version","alias_value":"1704.01318v1","created_at":"2026-05-18T00:46:58.473397+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1704.01318","created_at":"2026-05-18T00:46:58.473397+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZY2GV3PQBJI6","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZY2GV3PQBJI6VNMW","created_at":"2026-05-18T12:31:59.375834+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZY2GV3PQ","created_at":"2026-05-18T12:31:59.375834+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/ZY2GV3PQBJI6VNMWBX5BZNJABW","json":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW.json","graph_json":"https://pith.science/api/pith-number/ZY2GV3PQBJI6VNMWBX5BZNJABW/graph.json","events_json":"https://pith.science/api/pith-number/ZY2GV3PQBJI6VNMWBX5BZNJABW/events.json","paper":"https://pith.science/paper/ZY2GV3PQ"},"agent_actions":{"view_html":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW","download_json":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW.json","view_paper":"https://pith.science/paper/ZY2GV3PQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1704.01318&json=true","fetch_graph":"https://pith.science/api/pith-number/ZY2GV3PQBJI6VNMWBX5BZNJABW/graph.json","fetch_events":"https://pith.science/api/pith-number/ZY2GV3PQBJI6VNMWBX5BZNJABW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW/action/storage_attestation","attest_author":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW/action/author_attestation","sign_citation":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW/action/citation_signature","submit_replication":"https://pith.science/pith/ZY2GV3PQBJI6VNMWBX5BZNJABW/action/replication_record"}},"created_at":"2026-05-18T00:46:58.473397+00:00","updated_at":"2026-05-18T00:46:58.473397+00:00"}