{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:Z5BMKGOH6NRHVQ2HTQYQ5OBMD6","short_pith_number":"pith:Z5BMKGOH","schema_version":"1.0","canonical_sha256":"cf42c519c7f3627ac3479c310eb82c1f9aaa0bb6f9f57d21e9b0f40dc1b23d46","source":{"kind":"arxiv","id":"2111.09166","version":1},"attestation_state":"computed","paper":{"title":"RTGW2020: A powerful implementation of DFT + Gutzwiller method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Hongming Weng, Shiyu Peng, Xi Dai","submitted_at":"2021-11-17T14:56:28Z","abstract_excerpt":"In the present paper, we propose an efficient numerical scheme for Gutzwiller method for multi-band Hubbard models with general onsite Coulomb interaction. Following the basic idea of Deng et al. [Phys. Rev. B 79, 075114 (2009)] and extensions by Lanata et al. [Phys. Rev. B 85, 035133 (2012)], the ground state is variationally determined through optimizing the total energy with respect to the variational single particle density matrix (n0), which is called \"outer loop\". In the corresponding \"inner loop\" where n0 is fixed, the non-interacting wave function and the parameters contained in the Gu"},"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":"2111.09166","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.str-el","submitted_at":"2021-11-17T14:56:28Z","cross_cats_sorted":[],"title_canon_sha256":"79442a1be55c98399db99213b43e8c8c60edac2efe0bcea5210add7ad57d4543","abstract_canon_sha256":"df4b9541438332790bc22d1fd0b179f49664824aa378fcba5faaecf7c1ad0986"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:32:58.444376Z","signature_b64":"XkvafzSJFaDdcaLV03XIL/sRoG9BTSHKwpEI41pf3azKcb+A5CxTxFrUymrx6DWMMU1aWoOzG8HfMswaJGfXCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cf42c519c7f3627ac3479c310eb82c1f9aaa0bb6f9f57d21e9b0f40dc1b23d46","last_reissued_at":"2026-07-05T03:32:58.443968Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:32:58.443968Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"RTGW2020: A powerful implementation of DFT + Gutzwiller method","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"cond-mat.str-el","authors_text":"Hongming Weng, Shiyu Peng, Xi Dai","submitted_at":"2021-11-17T14:56:28Z","abstract_excerpt":"In the present paper, we propose an efficient numerical scheme for Gutzwiller method for multi-band Hubbard models with general onsite Coulomb interaction. Following the basic idea of Deng et al. [Phys. Rev. B 79, 075114 (2009)] and extensions by Lanata et al. [Phys. Rev. B 85, 035133 (2012)], the ground state is variationally determined through optimizing the total energy with respect to the variational single particle density matrix (n0), which is called \"outer loop\". In the corresponding \"inner loop\" where n0 is fixed, the non-interacting wave function and the parameters contained in the Gu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.09166","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2111.09166/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":"2111.09166","created_at":"2026-07-05T03:32:58.444027+00:00"},{"alias_kind":"arxiv_version","alias_value":"2111.09166v1","created_at":"2026-07-05T03:32:58.444027+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.09166","created_at":"2026-07-05T03:32:58.444027+00:00"},{"alias_kind":"pith_short_12","alias_value":"Z5BMKGOH6NRH","created_at":"2026-07-05T03:32:58.444027+00:00"},{"alias_kind":"pith_short_16","alias_value":"Z5BMKGOH6NRHVQ2H","created_at":"2026-07-05T03:32:58.444027+00:00"},{"alias_kind":"pith_short_8","alias_value":"Z5BMKGOH","created_at":"2026-07-05T03:32:58.444027+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/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6","json":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6.json","graph_json":"https://pith.science/api/pith-number/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/graph.json","events_json":"https://pith.science/api/pith-number/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/events.json","paper":"https://pith.science/paper/Z5BMKGOH"},"agent_actions":{"view_html":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6","download_json":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6.json","view_paper":"https://pith.science/paper/Z5BMKGOH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2111.09166&json=true","fetch_graph":"https://pith.science/api/pith-number/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/graph.json","fetch_events":"https://pith.science/api/pith-number/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/action/storage_attestation","attest_author":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/action/author_attestation","sign_citation":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/action/citation_signature","submit_replication":"https://pith.science/pith/Z5BMKGOH6NRHVQ2HTQYQ5OBMD6/action/replication_record"}},"created_at":"2026-07-05T03:32:58.444027+00:00","updated_at":"2026-07-05T03:32:58.444027+00:00"}