{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:WMQHAZ3FEWPBJW2S5LUJB5QIO2","short_pith_number":"pith:WMQHAZ3F","schema_version":"1.0","canonical_sha256":"b320706765259e14db52eae890f60876b118c96748c0cf74a08f0c4e24f411d7","source":{"kind":"arxiv","id":"1001.5051","version":2},"attestation_state":"computed","paper":{"title":"Interplane charge dynamics in a valence-bond dynamical mean-field theory of cuprate superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Georges, D. N. Basov, G. Kotliar, M. Ferrero, O. Parcollet","submitted_at":"2010-01-27T22:00:16Z","abstract_excerpt":"We present calculations of the interplane charge dynamics in the normal state of cuprate superconductors within the valence-bond dynamical mean-field theory. We show that by varying the hole doping, the c-axis optical conductivity and resistivity dramatically change character, going from metallic-like at large doping to insulating-like at low-doping. We establish a clear connection between the behavior of the c-axis optical and transport properties and the destruction of coherent quasiparticles as the pseudogap opens in the antinodal region of the Brillouin zone at low doping. We show that our"},"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":"1001.5051","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2010-01-27T22:00:16Z","cross_cats_sorted":[],"title_canon_sha256":"8ca694525e659d66b0c0ab92199e2a4dead65f050f62ed95944deb1a5ff930df","abstract_canon_sha256":"66c7730138c70d4d7e4dac7fd16b4484f73877190a2321dc424ede699d70e21d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:40:46.409977Z","signature_b64":"2kn/YKSU+0U6njniyZo+Xyb0w+xbXsKy0dmmmIXNlDhyOoX2AoTx9k87gGBFVbH3NlPIHGt+B0twOMKQfygYAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b320706765259e14db52eae890f60876b118c96748c0cf74a08f0c4e24f411d7","last_reissued_at":"2026-05-18T04:40:46.409311Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:40:46.409311Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Interplane charge dynamics in a valence-bond dynamical mean-field theory of cuprate superconductors","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"A. Georges, D. N. Basov, G. Kotliar, M. Ferrero, O. Parcollet","submitted_at":"2010-01-27T22:00:16Z","abstract_excerpt":"We present calculations of the interplane charge dynamics in the normal state of cuprate superconductors within the valence-bond dynamical mean-field theory. We show that by varying the hole doping, the c-axis optical conductivity and resistivity dramatically change character, going from metallic-like at large doping to insulating-like at low-doping. We establish a clear connection between the behavior of the c-axis optical and transport properties and the destruction of coherent quasiparticles as the pseudogap opens in the antinodal region of the Brillouin zone at low doping. We show that our"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1001.5051","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":"1001.5051","created_at":"2026-05-18T04:40:46.409418+00:00"},{"alias_kind":"arxiv_version","alias_value":"1001.5051v2","created_at":"2026-05-18T04:40:46.409418+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1001.5051","created_at":"2026-05-18T04:40:46.409418+00:00"},{"alias_kind":"pith_short_12","alias_value":"WMQHAZ3FEWPB","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"WMQHAZ3FEWPBJW2S","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"WMQHAZ3F","created_at":"2026-05-18T12:26:15.391820+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/WMQHAZ3FEWPBJW2S5LUJB5QIO2","json":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2.json","graph_json":"https://pith.science/api/pith-number/WMQHAZ3FEWPBJW2S5LUJB5QIO2/graph.json","events_json":"https://pith.science/api/pith-number/WMQHAZ3FEWPBJW2S5LUJB5QIO2/events.json","paper":"https://pith.science/paper/WMQHAZ3F"},"agent_actions":{"view_html":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2","download_json":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2.json","view_paper":"https://pith.science/paper/WMQHAZ3F","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1001.5051&json=true","fetch_graph":"https://pith.science/api/pith-number/WMQHAZ3FEWPBJW2S5LUJB5QIO2/graph.json","fetch_events":"https://pith.science/api/pith-number/WMQHAZ3FEWPBJW2S5LUJB5QIO2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2/action/storage_attestation","attest_author":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2/action/author_attestation","sign_citation":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2/action/citation_signature","submit_replication":"https://pith.science/pith/WMQHAZ3FEWPBJW2S5LUJB5QIO2/action/replication_record"}},"created_at":"2026-05-18T04:40:46.409418+00:00","updated_at":"2026-05-18T04:40:46.409418+00:00"}