{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:7Y5QJQW4D5PKGH6HS2FWJ5X7CG","short_pith_number":"pith:7Y5QJQW4","canonical_record":{"source":{"id":"1311.7573","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-11-29T14:16:41Z","cross_cats_sorted":[],"title_canon_sha256":"f6c661c850f5e91a9e095803b1c0639297266ec79f5fb3fc5a735cd2f146f300","abstract_canon_sha256":"e7bda25e905abf0803193654ea50a4b46b393a98bcbbbe4d14f9a2074120b645"},"schema_version":"1.0"},"canonical_sha256":"fe3b04c2dc1f5ea31fc7968b64f6ff11aaf3948c0de3e07146870ee7daa6e91f","source":{"kind":"arxiv","id":"1311.7573","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.7573","created_at":"2026-05-18T01:46:04Z"},{"alias_kind":"arxiv_version","alias_value":"1311.7573v1","created_at":"2026-05-18T01:46:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.7573","created_at":"2026-05-18T01:46:04Z"},{"alias_kind":"pith_short_12","alias_value":"7Y5QJQW4D5PK","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"7Y5QJQW4D5PKGH6H","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"7Y5QJQW4","created_at":"2026-05-18T12:27:38Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:7Y5QJQW4D5PKGH6HS2FWJ5X7CG","target":"record","payload":{"canonical_record":{"source":{"id":"1311.7573","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-11-29T14:16:41Z","cross_cats_sorted":[],"title_canon_sha256":"f6c661c850f5e91a9e095803b1c0639297266ec79f5fb3fc5a735cd2f146f300","abstract_canon_sha256":"e7bda25e905abf0803193654ea50a4b46b393a98bcbbbe4d14f9a2074120b645"},"schema_version":"1.0"},"canonical_sha256":"fe3b04c2dc1f5ea31fc7968b64f6ff11aaf3948c0de3e07146870ee7daa6e91f","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:46:04.814857Z","signature_b64":"ziq/UiAFVM4HgkeDtj1lyTC9lSDco2kNl1cVpHAC/zqA6h8iRGr0VCZcpcRa6hQiQqmZnDpZaUxoCL5b9zw9AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fe3b04c2dc1f5ea31fc7968b64f6ff11aaf3948c0de3e07146870ee7daa6e91f","last_reissued_at":"2026-05-18T01:46:04.814509Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:46:04.814509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1311.7573","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:46:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"U5IoZMD69JfLMeqRUwI+iwZS25625UzzWJR0hyvAqCqlt87NUo38wrA3eulou9Ic4nXHkM1a+BTtFTR3UkKADA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:33:42.446743Z"},"content_sha256":"d7725a41a7435dd4b12d4724ba5add56a3a01c612e0e41699c0372b5ee83d485","schema_version":"1.0","event_id":"sha256:d7725a41a7435dd4b12d4724ba5add56a3a01c612e0e41699c0372b5ee83d485"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:7Y5QJQW4D5PKGH6HS2FWJ5X7CG","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Large amplitude pairing fluctuations in atomic nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Luis Egido, Nuria L\\'opez Vaquero, Tom\\'as R. Rodr\\'iguez","submitted_at":"2013-11-29T14:16:41Z","abstract_excerpt":"Pairing fluctuations are self-consistently incorporated on the same footing as the quadrupole deformations in present state of the art calculations including particle number and angular momentum conservation as well as configuration mixing. The approach is complemented by the use of the finite range density dependent Gogny force which, with a unique source for the particle-hole and particle-particle interactions, guarantees a self-consistent interplay in both channels.\n  We have applied our formalism to study the role of the pairing degree of freedom in the description of the most relevant obs"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.7573","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":""},"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":"2026-05-18T01:46:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"h6BzlOgt0yWNqM0njZgug2ztwdlonlEznwrSm77m8fK9d9xH/svPm5iEsfI70zrzmRvmv0Yq/CEUEuq/XYcICg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T13:33:42.447091Z"},"content_sha256":"2b005311cac8d0d10c800cd27066a705aec17f7e4e32e4759944841d8f0c8b36","schema_version":"1.0","event_id":"sha256:2b005311cac8d0d10c800cd27066a705aec17f7e4e32e4759944841d8f0c8b36"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7Y5QJQW4D5PKGH6HS2FWJ5X7CG/bundle.json","state_url":"https://pith.science/pith/7Y5QJQW4D5PKGH6HS2FWJ5X7CG/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7Y5QJQW4D5PKGH6HS2FWJ5X7CG/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":"2026-06-01T13:33:42Z","links":{"resolver":"https://pith.science/pith/7Y5QJQW4D5PKGH6HS2FWJ5X7CG","bundle":"https://pith.science/pith/7Y5QJQW4D5PKGH6HS2FWJ5X7CG/bundle.json","state":"https://pith.science/pith/7Y5QJQW4D5PKGH6HS2FWJ5X7CG/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7Y5QJQW4D5PKGH6HS2FWJ5X7CG/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:7Y5QJQW4D5PKGH6HS2FWJ5X7CG","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":"e7bda25e905abf0803193654ea50a4b46b393a98bcbbbe4d14f9a2074120b645","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-11-29T14:16:41Z","title_canon_sha256":"f6c661c850f5e91a9e095803b1c0639297266ec79f5fb3fc5a735cd2f146f300"},"schema_version":"1.0","source":{"id":"1311.7573","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1311.7573","created_at":"2026-05-18T01:46:04Z"},{"alias_kind":"arxiv_version","alias_value":"1311.7573v1","created_at":"2026-05-18T01:46:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1311.7573","created_at":"2026-05-18T01:46:04Z"},{"alias_kind":"pith_short_12","alias_value":"7Y5QJQW4D5PK","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_16","alias_value":"7Y5QJQW4D5PKGH6H","created_at":"2026-05-18T12:27:38Z"},{"alias_kind":"pith_short_8","alias_value":"7Y5QJQW4","created_at":"2026-05-18T12:27:38Z"}],"graph_snapshots":[{"event_id":"sha256:2b005311cac8d0d10c800cd27066a705aec17f7e4e32e4759944841d8f0c8b36","target":"graph","created_at":"2026-05-18T01:46:04Z","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":"Pairing fluctuations are self-consistently incorporated on the same footing as the quadrupole deformations in present state of the art calculations including particle number and angular momentum conservation as well as configuration mixing. The approach is complemented by the use of the finite range density dependent Gogny force which, with a unique source for the particle-hole and particle-particle interactions, guarantees a self-consistent interplay in both channels.\n  We have applied our formalism to study the role of the pairing degree of freedom in the description of the most relevant obs","authors_text":"J. Luis Egido, Nuria L\\'opez Vaquero, Tom\\'as R. Rodr\\'iguez","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-11-29T14:16:41Z","title":"Large amplitude pairing fluctuations in atomic nuclei"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1311.7573","kind":"arxiv","version":1},"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:d7725a41a7435dd4b12d4724ba5add56a3a01c612e0e41699c0372b5ee83d485","target":"record","created_at":"2026-05-18T01:46:04Z","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":"e7bda25e905abf0803193654ea50a4b46b393a98bcbbbe4d14f9a2074120b645","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-11-29T14:16:41Z","title_canon_sha256":"f6c661c850f5e91a9e095803b1c0639297266ec79f5fb3fc5a735cd2f146f300"},"schema_version":"1.0","source":{"id":"1311.7573","kind":"arxiv","version":1}},"canonical_sha256":"fe3b04c2dc1f5ea31fc7968b64f6ff11aaf3948c0de3e07146870ee7daa6e91f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fe3b04c2dc1f5ea31fc7968b64f6ff11aaf3948c0de3e07146870ee7daa6e91f","first_computed_at":"2026-05-18T01:46:04.814509Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:46:04.814509Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ziq/UiAFVM4HgkeDtj1lyTC9lSDco2kNl1cVpHAC/zqA6h8iRGr0VCZcpcRa6hQiQqmZnDpZaUxoCL5b9zw9AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:46:04.814857Z","signed_message":"canonical_sha256_bytes"},"source_id":"1311.7573","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d7725a41a7435dd4b12d4724ba5add56a3a01c612e0e41699c0372b5ee83d485","sha256:2b005311cac8d0d10c800cd27066a705aec17f7e4e32e4759944841d8f0c8b36"],"state_sha256":"fbc2d00ba40cd2bc5b66d0ae0b7adfdbddd5e7751387826f1cbb349dbf1c6dbf"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bGyNN6WETWvSl6kSNoyvSC7SExwH5+RvqH4IdJpF/MsBK9cEROcss/RdLC+DmBXWoQQF76Mk5AW2Jz6eD7nZCA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T13:33:42.448993Z","bundle_sha256":"85c452acf6857399042f30529df21a442fa2b80f50c0b0817a9bd0f21ab3b47a"}}