{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:HDSDKODTIGZLCYCX4OILXCKCIG","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"496861cb05759cc51a61d49a16fe4c1b935e773060a2c7b6c61f1f37d2ff7b03","cross_cats_sorted":["cond-mat.mtrl-sci","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2013-11-14T15:39:35Z","title_canon_sha256":"bc82ebd44eeeb9dda81196f685b051edf08b064208b7bd31f14448e813f143d0"},"schema_version":"1.0","source":{"id":"1311.3544","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.3544","created_at":"2026-05-18T02:56:58Z"},{"alias_kind":"arxiv_version","alias_value":"1311.3544v3","created_at":"2026-05-18T02:56:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.3544","created_at":"2026-05-18T02:56:58Z"},{"alias_kind":"pith_short_12","alias_value":"HDSDKODTIGZL","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_16","alias_value":"HDSDKODTIGZLCYCX","created_at":"2026-05-18T12:27:46Z"},{"alias_kind":"pith_short_8","alias_value":"HDSDKODT","created_at":"2026-05-18T12:27:46Z"}],"graph_snapshots":[{"event_id":"sha256:ba670fe6c8a4f2080548c154cfc507dd64f6fdc92a94a44dee9d91ffeb2326e2","target":"graph","created_at":"2026-05-18T02:56:58Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"Recently, we have demonstrated that the problems finding a suitable adiabatic approximation in time-dependent one-body reduced density matrix functional theory can be remedied by introducing an additional degree of freedom to describe the system: the phase of the natural orbitals [Phys. Rev. Lett. 105, 013002 (2010), J. Chem. Phys. 133, 174119 (2010)]. In this article we will show in detail how the frequency-dependent response equations give the proper static limit ($\\omega\\to0$), including the perturbation in the chemical potential, which is required in static response theory to ensure the co","authors_text":"Evert Jan Baerends, Klaas J. H. Giesbertz, Oleg V. Gritsenko","cross_cats":["cond-mat.mtrl-sci","quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2013-11-14T15:39:35Z","title":"Response calculations based on an independent particle system with the exact one-particle density matrix: polarizabilities"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.3544","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:8a9bd2b122a38db8c213d868a3f13acfbf9bdcd46243e1f63859f4503d26aaf9","target":"record","created_at":"2026-05-18T02:56:58Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"496861cb05759cc51a61d49a16fe4c1b935e773060a2c7b6c61f1f37d2ff7b03","cross_cats_sorted":["cond-mat.mtrl-sci","quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2013-11-14T15:39:35Z","title_canon_sha256":"bc82ebd44eeeb9dda81196f685b051edf08b064208b7bd31f14448e813f143d0"},"schema_version":"1.0","source":{"id":"1311.3544","kind":"arxiv","version":3}},"canonical_sha256":"38e435387341b2b16057e390bb8942419de01062c3d6381afbed58af10384640","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"38e435387341b2b16057e390bb8942419de01062c3d6381afbed58af10384640","first_computed_at":"2026-05-18T02:56:58.286574Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:56:58.286574Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"L0P/w6EZwkT7aZP5A317JYWUsvD4PSiGSKHf2bwRYplbXKWlDnAOuYGeGiH2LILPJ0X8xoQsgAbZkEIFZU0pAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:56:58.286966Z","signed_message":"canonical_sha256_bytes"},"source_id":"1311.3544","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8a9bd2b122a38db8c213d868a3f13acfbf9bdcd46243e1f63859f4503d26aaf9","sha256:ba670fe6c8a4f2080548c154cfc507dd64f6fdc92a94a44dee9d91ffeb2326e2"],"state_sha256":"338ffbfe9293665be89407a2f5f461791fc5f4f580941c2d7dcc7403073be6d9"}