{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:FDU7FS4RCZ5XQZNOSFS4OUONIX","short_pith_number":"pith:FDU7FS4R","schema_version":"1.0","canonical_sha256":"28e9f2cb91167b7865ae9165c751cd45c664bbeae8856cbd9ae2314ee6424bcc","source":{"kind":"arxiv","id":"2310.04613","version":4},"attestation_state":"computed","paper":{"title":"ComDMFT v.2.0: Fully Self-Consistent ab initio GW+EDMFT for the Electronic Structure of Correlated Quantum Materials","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"Byungkyun Kang, Corey Melnick, Gabriel Kotliar, Hoonkyung Lee, Mancheon Han, Patrick Semon, Sangkook Choi, Seongjun Mo","submitted_at":"2023-10-06T22:11:40Z","abstract_excerpt":"ComDMFT is a parallel computational package designed to study the electronic structure of correlated quantum materials from first principles. Our approach is based on the combination of first-principles methods and dynamical mean field theories. In version 2.0, we implemented fully-diagrammatic GW+EDMFT from first-principles. In this approach, correlated electrons are treated within full GW+EDMFT and the rest are treated within full-GW, seamlessly. This implementation enables the electronic structure calculation of quantum materials with weak, intermediate, and strong electron correlation with"},"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":"2310.04613","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"cond-mat.str-el","submitted_at":"2023-10-06T22:11:40Z","cross_cats_sorted":["cond-mat.mtrl-sci"],"title_canon_sha256":"3ef52671c73fb49d1dfbe2ac7651a8aa12314a0ff2f81a2fe0f4ad29e93a053c","abstract_canon_sha256":"3572329efd2e44de59d40baa8e389fb2a184f1eafd7883d4943f8a7dd597db97"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:35:46.420855Z","signature_b64":"QwqbMXSCFT8L+5w/84mek5yhvbg7gj3NN/ExVWh47nIfXYDw0RXbSQ1ga6aAUKD91pqL+Ubccw9Jd6WhqYukBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"28e9f2cb91167b7865ae9165c751cd45c664bbeae8856cbd9ae2314ee6424bcc","last_reissued_at":"2026-07-05T09:35:46.420342Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:35:46.420342Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"ComDMFT v.2.0: Fully Self-Consistent ab initio GW+EDMFT for the Electronic Structure of Correlated Quantum Materials","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.mtrl-sci"],"primary_cat":"cond-mat.str-el","authors_text":"Byungkyun Kang, Corey Melnick, Gabriel Kotliar, Hoonkyung Lee, Mancheon Han, Patrick Semon, Sangkook Choi, Seongjun Mo","submitted_at":"2023-10-06T22:11:40Z","abstract_excerpt":"ComDMFT is a parallel computational package designed to study the electronic structure of correlated quantum materials from first principles. Our approach is based on the combination of first-principles methods and dynamical mean field theories. In version 2.0, we implemented fully-diagrammatic GW+EDMFT from first-principles. In this approach, correlated electrons are treated within full GW+EDMFT and the rest are treated within full-GW, seamlessly. This implementation enables the electronic structure calculation of quantum materials with weak, intermediate, and strong electron correlation with"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2310.04613","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2310.04613/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2310.04613","created_at":"2026-07-05T09:35:46.420403+00:00"},{"alias_kind":"arxiv_version","alias_value":"2310.04613v4","created_at":"2026-07-05T09:35:46.420403+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2310.04613","created_at":"2026-07-05T09:35:46.420403+00:00"},{"alias_kind":"pith_short_12","alias_value":"FDU7FS4RCZ5X","created_at":"2026-07-05T09:35:46.420403+00:00"},{"alias_kind":"pith_short_16","alias_value":"FDU7FS4RCZ5XQZNO","created_at":"2026-07-05T09:35:46.420403+00:00"},{"alias_kind":"pith_short_8","alias_value":"FDU7FS4R","created_at":"2026-07-05T09:35:46.420403+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2502.03646","citing_title":"Coexistence of 3D and quasi-2D Fermi surfaces driven by orbital selective Kondo scattering in UTe$_2$","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX","json":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX.json","graph_json":"https://pith.science/api/pith-number/FDU7FS4RCZ5XQZNOSFS4OUONIX/graph.json","events_json":"https://pith.science/api/pith-number/FDU7FS4RCZ5XQZNOSFS4OUONIX/events.json","paper":"https://pith.science/paper/FDU7FS4R"},"agent_actions":{"view_html":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX","download_json":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX.json","view_paper":"https://pith.science/paper/FDU7FS4R","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2310.04613&json=true","fetch_graph":"https://pith.science/api/pith-number/FDU7FS4RCZ5XQZNOSFS4OUONIX/graph.json","fetch_events":"https://pith.science/api/pith-number/FDU7FS4RCZ5XQZNOSFS4OUONIX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX/action/storage_attestation","attest_author":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX/action/author_attestation","sign_citation":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX/action/citation_signature","submit_replication":"https://pith.science/pith/FDU7FS4RCZ5XQZNOSFS4OUONIX/action/replication_record"}},"created_at":"2026-07-05T09:35:46.420403+00:00","updated_at":"2026-07-05T09:35:46.420403+00:00"}