{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1995:73ZQ53DRYMG6SBUV4KRTO7JMFG","short_pith_number":"pith:73ZQ53DR","schema_version":"1.0","canonical_sha256":"fef30eec71c30de90695e2a3377d2c298224b88136b078d2543cd4e4b80ff9e3","source":{"kind":"arxiv","id":"cond-mat/9502097","version":1},"attestation_state":"computed","paper":{"title":"The motion of holes on the triangular lattice: t-J model","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Mohamed Azzouz, Thierry Dombre","submitted_at":"1995-02-23T18:09:30Z","abstract_excerpt":"The motion of holes on the triangular lattice is studied using the t-J model. Within the Born self-consistent approximation and the exact Lanczos diagonalization, the single hole physics is first analyzed. Then the spiral theory of Shraiman and Siggia is used to investigate the case of a finite density of holes."},"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":"cond-mat/9502097","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"cond-mat","submitted_at":"1995-02-23T18:09:30Z","cross_cats_sorted":[],"title_canon_sha256":"2bac8737712bfd4c2641ec3eeeadcac06c684f3b56c597f524fdf361cf37fd0b","abstract_canon_sha256":"270631778c6842c223e0d373e66bfc7985d286d338c21306e23a3fbad1fb4c6c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:07:11.974219Z","signature_b64":"3i+1i2UxHy05IWCTsE7+d2PFUFVoX6A9Op6q+7+loajeTMIqY2DDIxuD4uTyuPE/yufers0Qes737H9qq94iAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fef30eec71c30de90695e2a3377d2c298224b88136b078d2543cd4e4b80ff9e3","last_reissued_at":"2026-05-18T01:07:11.973646Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:07:11.973646Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The motion of holes on the triangular lattice: t-J model","license":"","headline":"","cross_cats":[],"primary_cat":"cond-mat","authors_text":"Mohamed Azzouz, Thierry Dombre","submitted_at":"1995-02-23T18:09:30Z","abstract_excerpt":"The motion of holes on the triangular lattice is studied using the t-J model. Within the Born self-consistent approximation and the exact Lanczos diagonalization, the single hole physics is first analyzed. Then the spiral theory of Shraiman and Siggia is used to investigate the case of a finite density of holes."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"cond-mat/9502097","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":"cond-mat/9502097","created_at":"2026-05-18T01:07:11.973734+00:00"},{"alias_kind":"arxiv_version","alias_value":"cond-mat/9502097v1","created_at":"2026-05-18T01:07:11.973734+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.cond-mat/9502097","created_at":"2026-05-18T01:07:11.973734+00:00"},{"alias_kind":"pith_short_12","alias_value":"73ZQ53DRYMG6","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_16","alias_value":"73ZQ53DRYMG6SBUV","created_at":"2026-05-18T12:25:47.700082+00:00"},{"alias_kind":"pith_short_8","alias_value":"73ZQ53DR","created_at":"2026-05-18T12:25:47.700082+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/73ZQ53DRYMG6SBUV4KRTO7JMFG","json":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG.json","graph_json":"https://pith.science/api/pith-number/73ZQ53DRYMG6SBUV4KRTO7JMFG/graph.json","events_json":"https://pith.science/api/pith-number/73ZQ53DRYMG6SBUV4KRTO7JMFG/events.json","paper":"https://pith.science/paper/73ZQ53DR"},"agent_actions":{"view_html":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG","download_json":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG.json","view_paper":"https://pith.science/paper/73ZQ53DR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=cond-mat/9502097&json=true","fetch_graph":"https://pith.science/api/pith-number/73ZQ53DRYMG6SBUV4KRTO7JMFG/graph.json","fetch_events":"https://pith.science/api/pith-number/73ZQ53DRYMG6SBUV4KRTO7JMFG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG/action/storage_attestation","attest_author":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG/action/author_attestation","sign_citation":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG/action/citation_signature","submit_replication":"https://pith.science/pith/73ZQ53DRYMG6SBUV4KRTO7JMFG/action/replication_record"}},"created_at":"2026-05-18T01:07:11.973734+00:00","updated_at":"2026-05-18T01:07:11.973734+00:00"}