{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:TUJDZ2Y3P3IDXPOVKRA3N7MXQD","short_pith_number":"pith:TUJDZ2Y3","schema_version":"1.0","canonical_sha256":"9d123ceb1b7ed03bbdd55441b6fd9780cbd3ac5e7a4dc6e6e2cc0506a4c5153c","source":{"kind":"arxiv","id":"1302.2221","version":2},"attestation_state":"computed","paper":{"title":"Hole-doping driven antiparallel magnetic order underlying the superconducting and pseudogap states in high-temperature cuprate superconductor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Takashi Uchino","submitted_at":"2013-02-09T11:23:45Z","abstract_excerpt":"Unveiling the nature of the pseudogap and its relation to both superconductivity and antiferromagnetic Mott insulators, the pairing mechanism, and a non-Fermi liquid phase is a key issue for understanding high temperature superconductivity in cuprates.We here show that antiparallel magnetic order can be reasonably and naturally predicted in hole-doped CuO2 planes by starting from the ground state of a weakly doped antiferromagnetic insulator, where a Skyrmion-type three-dimensional spin texture is created around the doped hole. The superconducting transition temperature Tc can be understood in"},"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":"1302.2221","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.supr-con","submitted_at":"2013-02-09T11:23:45Z","cross_cats_sorted":[],"title_canon_sha256":"3a834f70ec6b28b77c7b2efdc0e36cd44ec072c597526e03fb1a1b13ddaa5994","abstract_canon_sha256":"d0554e1935f31a5b8fd06e3f10ce32fe36688da2780f3b049e29090b6decabef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:33:49.369806Z","signature_b64":"rPqNr8sGLCIS97QvddLPPbWYGIVjBveHzePSMehWEYDWdzRdA+p6Wkze6yBFqIahGeHUtcnKiW1Kmm5NTiZeCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d123ceb1b7ed03bbdd55441b6fd9780cbd3ac5e7a4dc6e6e2cc0506a4c5153c","last_reissued_at":"2026-05-18T03:33:49.368981Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:33:49.368981Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hole-doping driven antiparallel magnetic order underlying the superconducting and pseudogap states in high-temperature cuprate superconductor","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.supr-con","authors_text":"Takashi Uchino","submitted_at":"2013-02-09T11:23:45Z","abstract_excerpt":"Unveiling the nature of the pseudogap and its relation to both superconductivity and antiferromagnetic Mott insulators, the pairing mechanism, and a non-Fermi liquid phase is a key issue for understanding high temperature superconductivity in cuprates.We here show that antiparallel magnetic order can be reasonably and naturally predicted in hole-doped CuO2 planes by starting from the ground state of a weakly doped antiferromagnetic insulator, where a Skyrmion-type three-dimensional spin texture is created around the doped hole. The superconducting transition temperature Tc can be understood in"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1302.2221","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":"1302.2221","created_at":"2026-05-18T03:33:49.369119+00:00"},{"alias_kind":"arxiv_version","alias_value":"1302.2221v2","created_at":"2026-05-18T03:33:49.369119+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1302.2221","created_at":"2026-05-18T03:33:49.369119+00:00"},{"alias_kind":"pith_short_12","alias_value":"TUJDZ2Y3P3ID","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_16","alias_value":"TUJDZ2Y3P3IDXPOV","created_at":"2026-05-18T12:28:02.375192+00:00"},{"alias_kind":"pith_short_8","alias_value":"TUJDZ2Y3","created_at":"2026-05-18T12:28:02.375192+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/TUJDZ2Y3P3IDXPOVKRA3N7MXQD","json":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD.json","graph_json":"https://pith.science/api/pith-number/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/graph.json","events_json":"https://pith.science/api/pith-number/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/events.json","paper":"https://pith.science/paper/TUJDZ2Y3"},"agent_actions":{"view_html":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD","download_json":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD.json","view_paper":"https://pith.science/paper/TUJDZ2Y3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1302.2221&json=true","fetch_graph":"https://pith.science/api/pith-number/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/graph.json","fetch_events":"https://pith.science/api/pith-number/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/action/storage_attestation","attest_author":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/action/author_attestation","sign_citation":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/action/citation_signature","submit_replication":"https://pith.science/pith/TUJDZ2Y3P3IDXPOVKRA3N7MXQD/action/replication_record"}},"created_at":"2026-05-18T03:33:49.369119+00:00","updated_at":"2026-05-18T03:33:49.369119+00:00"}