{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:3HFNC6SWH7TNUM7H3XZ5AYULFC","short_pith_number":"pith:3HFNC6SW","canonical_record":{"source":{"id":"1810.11249","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-10-26T10:22:32Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"1028547605244dcce73758cfb70d71d404b755d7de7a80e434f2eca220e0861e","abstract_canon_sha256":"2ed74c5f718cba8e6e3ace14b4483594fd71682276c0435fa4a32acb59c20fdb"},"schema_version":"1.0"},"canonical_sha256":"d9cad17a563fe6da33e7ddf3d0628b28b966c609a35bf4a3c100255f08a26dbe","source":{"kind":"arxiv","id":"1810.11249","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.11249","created_at":"2026-05-17T23:50:38Z"},{"alias_kind":"arxiv_version","alias_value":"1810.11249v2","created_at":"2026-05-17T23:50:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.11249","created_at":"2026-05-17T23:50:38Z"},{"alias_kind":"pith_short_12","alias_value":"3HFNC6SWH7TN","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"3HFNC6SWH7TNUM7H","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"3HFNC6SW","created_at":"2026-05-18T12:32:02Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:3HFNC6SWH7TNUM7H3XZ5AYULFC","target":"record","payload":{"canonical_record":{"source":{"id":"1810.11249","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-10-26T10:22:32Z","cross_cats_sorted":["cond-mat.str-el"],"title_canon_sha256":"1028547605244dcce73758cfb70d71d404b755d7de7a80e434f2eca220e0861e","abstract_canon_sha256":"2ed74c5f718cba8e6e3ace14b4483594fd71682276c0435fa4a32acb59c20fdb"},"schema_version":"1.0"},"canonical_sha256":"d9cad17a563fe6da33e7ddf3d0628b28b966c609a35bf4a3c100255f08a26dbe","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:50:38.406489Z","signature_b64":"KOannROBVyiS31MIwF1Jxp8DuHdsxmLw2qDazJXtpZAMRmg8FcLzReLUHO8CFb6mlt99JcqfBmmbIEyruyBbBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d9cad17a563fe6da33e7ddf3d0628b28b966c609a35bf4a3c100255f08a26dbe","last_reissued_at":"2026-05-17T23:50:38.405982Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:50:38.405982Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1810.11249","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":"2026-05-17T23:50:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"I9jvmNfT+oONml3XxO5pnVRFd7kSjWSBKh36ijX6J1Yz25uCtNUh6gkW+lFXzk0BYBu8AeGA0Tht/3me8ky5AQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:25:34.008299Z"},"content_sha256":"a3c23550cb8fa3b6b147976f9a517397c317749f40abc3b8c73ec9fed84985cd","schema_version":"1.0","event_id":"sha256:a3c23550cb8fa3b6b147976f9a517397c317749f40abc3b8c73ec9fed84985cd"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:3HFNC6SWH7TNUM7H3XZ5AYULFC","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strong-interaction limit of an adiabatic connection in Hartree-Fock theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el"],"primary_cat":"physics.chem-ph","authors_text":"Eduardo Fabiano, Michael Seidl, Paola Gori-Giorgi, Sara Giarrusso, Stefan Vuckovic","submitted_at":"2018-10-26T10:22:32Z","abstract_excerpt":"We show that the leading term in the strong-interaction limit of the adiabatic connection that has as weak-interaction expansion the Moeller-Plesset perturbation theory can be fully determined from a functional of the Hartree-Fock density. We analyze this functional and highlight similarities and differences with the strong-interaction limit of the density-fixed adiabatic connection case of Kohn-Sham density functional theory."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.11249","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":"2026-05-17T23:50:38Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"EiEeY/SGQHelEhFZSDJU6hPwExQEe4lU7V2JS9zpvn0YovErPp6+w3VtiwgEivAGDZM26zjaSNDGc/1nAP+TBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-25T13:25:34.009028Z"},"content_sha256":"120227dd4f4f4e90e3bc083fe66fcdd9c4a40196cba79bf0b433ad1a8461af4a","schema_version":"1.0","event_id":"sha256:120227dd4f4f4e90e3bc083fe66fcdd9c4a40196cba79bf0b433ad1a8461af4a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3HFNC6SWH7TNUM7H3XZ5AYULFC/bundle.json","state_url":"https://pith.science/pith/3HFNC6SWH7TNUM7H3XZ5AYULFC/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3HFNC6SWH7TNUM7H3XZ5AYULFC/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":"2026-05-25T13:25:34Z","links":{"resolver":"https://pith.science/pith/3HFNC6SWH7TNUM7H3XZ5AYULFC","bundle":"https://pith.science/pith/3HFNC6SWH7TNUM7H3XZ5AYULFC/bundle.json","state":"https://pith.science/pith/3HFNC6SWH7TNUM7H3XZ5AYULFC/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3HFNC6SWH7TNUM7H3XZ5AYULFC/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:3HFNC6SWH7TNUM7H3XZ5AYULFC","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":"2ed74c5f718cba8e6e3ace14b4483594fd71682276c0435fa4a32acb59c20fdb","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-10-26T10:22:32Z","title_canon_sha256":"1028547605244dcce73758cfb70d71d404b755d7de7a80e434f2eca220e0861e"},"schema_version":"1.0","source":{"id":"1810.11249","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1810.11249","created_at":"2026-05-17T23:50:38Z"},{"alias_kind":"arxiv_version","alias_value":"1810.11249v2","created_at":"2026-05-17T23:50:38Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1810.11249","created_at":"2026-05-17T23:50:38Z"},{"alias_kind":"pith_short_12","alias_value":"3HFNC6SWH7TN","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_16","alias_value":"3HFNC6SWH7TNUM7H","created_at":"2026-05-18T12:32:02Z"},{"alias_kind":"pith_short_8","alias_value":"3HFNC6SW","created_at":"2026-05-18T12:32:02Z"}],"graph_snapshots":[{"event_id":"sha256:120227dd4f4f4e90e3bc083fe66fcdd9c4a40196cba79bf0b433ad1a8461af4a","target":"graph","created_at":"2026-05-17T23:50:38Z","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":"We show that the leading term in the strong-interaction limit of the adiabatic connection that has as weak-interaction expansion the Moeller-Plesset perturbation theory can be fully determined from a functional of the Hartree-Fock density. We analyze this functional and highlight similarities and differences with the strong-interaction limit of the density-fixed adiabatic connection case of Kohn-Sham density functional theory.","authors_text":"Eduardo Fabiano, Michael Seidl, Paola Gori-Giorgi, Sara Giarrusso, Stefan Vuckovic","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-10-26T10:22:32Z","title":"Strong-interaction limit of an adiabatic connection in Hartree-Fock theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1810.11249","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:a3c23550cb8fa3b6b147976f9a517397c317749f40abc3b8c73ec9fed84985cd","target":"record","created_at":"2026-05-17T23:50:38Z","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":"2ed74c5f718cba8e6e3ace14b4483594fd71682276c0435fa4a32acb59c20fdb","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.chem-ph","submitted_at":"2018-10-26T10:22:32Z","title_canon_sha256":"1028547605244dcce73758cfb70d71d404b755d7de7a80e434f2eca220e0861e"},"schema_version":"1.0","source":{"id":"1810.11249","kind":"arxiv","version":2}},"canonical_sha256":"d9cad17a563fe6da33e7ddf3d0628b28b966c609a35bf4a3c100255f08a26dbe","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d9cad17a563fe6da33e7ddf3d0628b28b966c609a35bf4a3c100255f08a26dbe","first_computed_at":"2026-05-17T23:50:38.405982Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-17T23:50:38.405982Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KOannROBVyiS31MIwF1Jxp8DuHdsxmLw2qDazJXtpZAMRmg8FcLzReLUHO8CFb6mlt99JcqfBmmbIEyruyBbBA==","signature_status":"signed_v1","signed_at":"2026-05-17T23:50:38.406489Z","signed_message":"canonical_sha256_bytes"},"source_id":"1810.11249","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:a3c23550cb8fa3b6b147976f9a517397c317749f40abc3b8c73ec9fed84985cd","sha256:120227dd4f4f4e90e3bc083fe66fcdd9c4a40196cba79bf0b433ad1a8461af4a"],"state_sha256":"5c0ef55077dbb8977d06657751e8172616b9d7e643340799f35735e111b6db68"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"jrl4Mujma59X7miJ7GxjAPCsC7m2i2J5he4b7rty53N8gr9v7zUfhMJkiDIW2DEHKs0NLtN/ExQvIRrRta2MDg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-25T13:25:34.012407Z","bundle_sha256":"45fffa0d65d368e0235afccfb975f120458027404d7dba971edf5af202692ecc"}}