{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:ZYPTDNE4FTA3XCLGUUP3ZBX6R3","short_pith_number":"pith:ZYPTDNE4","canonical_record":{"source":{"id":"1603.05385","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-03-17T08:15:08Z","cross_cats_sorted":[],"title_canon_sha256":"0ba5749e5fd8a1372815de12cef834d290ee6c49992289d05bc875b3fb26b48a","abstract_canon_sha256":"98a2cf911f5ddcfebc4bafa890210a9e85c5edf1703e6900e2ef1e342e988b2f"},"schema_version":"1.0"},"canonical_sha256":"ce1f31b49c2cc1bb8966a51fbc86fe8ef2b8342cd4f0bdbd73e69c23d2140c55","source":{"kind":"arxiv","id":"1603.05385","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.05385","created_at":"2026-05-18T01:10:45Z"},{"alias_kind":"arxiv_version","alias_value":"1603.05385v2","created_at":"2026-05-18T01:10:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.05385","created_at":"2026-05-18T01:10:45Z"},{"alias_kind":"pith_short_12","alias_value":"ZYPTDNE4FTA3","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"ZYPTDNE4FTA3XCLG","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"ZYPTDNE4","created_at":"2026-05-18T12:30:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:ZYPTDNE4FTA3XCLGUUP3ZBX6R3","target":"record","payload":{"canonical_record":{"source":{"id":"1603.05385","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-03-17T08:15:08Z","cross_cats_sorted":[],"title_canon_sha256":"0ba5749e5fd8a1372815de12cef834d290ee6c49992289d05bc875b3fb26b48a","abstract_canon_sha256":"98a2cf911f5ddcfebc4bafa890210a9e85c5edf1703e6900e2ef1e342e988b2f"},"schema_version":"1.0"},"canonical_sha256":"ce1f31b49c2cc1bb8966a51fbc86fe8ef2b8342cd4f0bdbd73e69c23d2140c55","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:45.664830Z","signature_b64":"P7ejQCTGLHe+8DImeRAD2xXR37vC6UmD5O7xpQYtm01dAmufyrpvHZ0dA6m4XbFLB/8I9w/OfwmJ1oFdhzdXCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ce1f31b49c2cc1bb8966a51fbc86fe8ef2b8342cd4f0bdbd73e69c23d2140c55","last_reissued_at":"2026-05-18T01:10:45.664372Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:45.664372Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1603.05385","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:10:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"RkyexWM3B+FZkh4PZ+44v4Ewmd4FJudRv3PFnW86O46N6Mabr/YlK6gxMyWtC71i480aUH1dYoMOy10xrQRADA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:01:24.617815Z"},"content_sha256":"5cfadce71a013b2b8734ed2d759486a97e91c2501929bdc8499d0ec306de3900","schema_version":"1.0","event_id":"sha256:5cfadce71a013b2b8734ed2d759486a97e91c2501929bdc8499d0ec306de3900"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:ZYPTDNE4FTA3XCLGUUP3ZBX6R3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Ghost interaction correction in ensemble density-functional theory for excited states with and without range separation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.chem-ph","authors_text":"Emmanuel Fromager, Md. Mehboob Alam, Stefan Knecht","submitted_at":"2016-03-17T08:15:08Z","abstract_excerpt":"Ensemble density-functional theory (eDFT) suffers from the so-called \"ghost interaction\" error when approximate exchange-correlation functionals are used. In this work, we present a rigorous ghost interaction correction (GIC) scheme in the context of range-separated eDFT. The method relies on an exact decomposition of the ensemble short-range exchange-correlation energy into a multideterminantal exact exchange term, which involves the long-range interacting ensemble density matrix instead of the Kohn--Sham (KS) one, and a complementary density-functional correlation energy. A generalized adiab"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.05385","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:10:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"WdiMl18ekuoBf0nN2DoTNQiGyofoS2BxnqfXPE5Bj62YFI6rjRYej5q9wgXwAbd43mvzo8h3rFWT5SAmiNMiCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T21:01:24.618508Z"},"content_sha256":"ed01ab16f2b8f808873c0a8d55b5e32a55f0c33cb73d4c3c79e1c0963133fc4d","schema_version":"1.0","event_id":"sha256:ed01ab16f2b8f808873c0a8d55b5e32a55f0c33cb73d4c3c79e1c0963133fc4d"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZYPTDNE4FTA3XCLGUUP3ZBX6R3/bundle.json","state_url":"https://pith.science/pith/ZYPTDNE4FTA3XCLGUUP3ZBX6R3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZYPTDNE4FTA3XCLGUUP3ZBX6R3/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-25T21:01:24Z","links":{"resolver":"https://pith.science/pith/ZYPTDNE4FTA3XCLGUUP3ZBX6R3","bundle":"https://pith.science/pith/ZYPTDNE4FTA3XCLGUUP3ZBX6R3/bundle.json","state":"https://pith.science/pith/ZYPTDNE4FTA3XCLGUUP3ZBX6R3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZYPTDNE4FTA3XCLGUUP3ZBX6R3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:ZYPTDNE4FTA3XCLGUUP3ZBX6R3","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":"98a2cf911f5ddcfebc4bafa890210a9e85c5edf1703e6900e2ef1e342e988b2f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-03-17T08:15:08Z","title_canon_sha256":"0ba5749e5fd8a1372815de12cef834d290ee6c49992289d05bc875b3fb26b48a"},"schema_version":"1.0","source":{"id":"1603.05385","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1603.05385","created_at":"2026-05-18T01:10:45Z"},{"alias_kind":"arxiv_version","alias_value":"1603.05385v2","created_at":"2026-05-18T01:10:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.05385","created_at":"2026-05-18T01:10:45Z"},{"alias_kind":"pith_short_12","alias_value":"ZYPTDNE4FTA3","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_16","alias_value":"ZYPTDNE4FTA3XCLG","created_at":"2026-05-18T12:30:55Z"},{"alias_kind":"pith_short_8","alias_value":"ZYPTDNE4","created_at":"2026-05-18T12:30:55Z"}],"graph_snapshots":[{"event_id":"sha256:ed01ab16f2b8f808873c0a8d55b5e32a55f0c33cb73d4c3c79e1c0963133fc4d","target":"graph","created_at":"2026-05-18T01:10:45Z","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":"Ensemble density-functional theory (eDFT) suffers from the so-called \"ghost interaction\" error when approximate exchange-correlation functionals are used. In this work, we present a rigorous ghost interaction correction (GIC) scheme in the context of range-separated eDFT. The method relies on an exact decomposition of the ensemble short-range exchange-correlation energy into a multideterminantal exact exchange term, which involves the long-range interacting ensemble density matrix instead of the Kohn--Sham (KS) one, and a complementary density-functional correlation energy. A generalized adiab","authors_text":"Emmanuel Fromager, Md. Mehboob Alam, Stefan Knecht","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-03-17T08:15:08Z","title":"Ghost interaction correction in ensemble density-functional theory for excited states with and without range separation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.05385","kind":"arxiv","version":2},"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":"sha256:5cfadce71a013b2b8734ed2d759486a97e91c2501929bdc8499d0ec306de3900","target":"record","created_at":"2026-05-18T01:10:45Z","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":"98a2cf911f5ddcfebc4bafa890210a9e85c5edf1703e6900e2ef1e342e988b2f","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2016-03-17T08:15:08Z","title_canon_sha256":"0ba5749e5fd8a1372815de12cef834d290ee6c49992289d05bc875b3fb26b48a"},"schema_version":"1.0","source":{"id":"1603.05385","kind":"arxiv","version":2}},"canonical_sha256":"ce1f31b49c2cc1bb8966a51fbc86fe8ef2b8342cd4f0bdbd73e69c23d2140c55","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ce1f31b49c2cc1bb8966a51fbc86fe8ef2b8342cd4f0bdbd73e69c23d2140c55","first_computed_at":"2026-05-18T01:10:45.664372Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:10:45.664372Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"P7ejQCTGLHe+8DImeRAD2xXR37vC6UmD5O7xpQYtm01dAmufyrpvHZ0dA6m4XbFLB/8I9w/OfwmJ1oFdhzdXCw==","signature_status":"signed_v1","signed_at":"2026-05-18T01:10:45.664830Z","signed_message":"canonical_sha256_bytes"},"source_id":"1603.05385","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5cfadce71a013b2b8734ed2d759486a97e91c2501929bdc8499d0ec306de3900","sha256:ed01ab16f2b8f808873c0a8d55b5e32a55f0c33cb73d4c3c79e1c0963133fc4d"],"state_sha256":"47edf9bf061f43df966fb7ca7953a9d765be2905c1c9876ad91affc8cd952c3f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yh+JZQwTcr+m6AYCdB0AsmRMvqjDES1ZO9cbXLU1ya2pejVauojyk7rx77cgefdLCBkbl2zrRaNS3xjPmEKhBg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T21:01:24.622614Z","bundle_sha256":"3c76fb598fd2cd0609415f97c6e429ef72c7ea600e30cb0ef14bd463f8917c2d"}}