{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2000:7Q5NDDUVQP4BXBILGOK575QQ73","short_pith_number":"pith:7Q5NDDUV","canonical_record":{"source":{"id":"nucl-th/0007052","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2000-07-24T12:28:54Z","cross_cats_sorted":[],"title_canon_sha256":"3c98f0d749cb1c6d0a89d63f070ac57be49f102046575ce1d26f4e7ef98b4d1b","abstract_canon_sha256":"86786a5cfa0862809c2530b788fb2f53328e725dc62a3734b3b0c816aca622e1"},"schema_version":"1.0"},"canonical_sha256":"fc3ad18e9583f81b850b3395dff610fed16f3876ffbfcfd93b4265a4686b42ab","source":{"kind":"arxiv","id":"nucl-th/0007052","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0007052","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0007052v1","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0007052","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"pith_short_12","alias_value":"7Q5NDDUVQP4B","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"pith_short_16","alias_value":"7Q5NDDUVQP4BXBIL","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"pith_short_8","alias_value":"7Q5NDDUV","created_at":"2026-07-04T16:22:04Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2000:7Q5NDDUVQP4BXBILGOK575QQ73","target":"record","payload":{"canonical_record":{"source":{"id":"nucl-th/0007052","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2000-07-24T12:28:54Z","cross_cats_sorted":[],"title_canon_sha256":"3c98f0d749cb1c6d0a89d63f070ac57be49f102046575ce1d26f4e7ef98b4d1b","abstract_canon_sha256":"86786a5cfa0862809c2530b788fb2f53328e725dc62a3734b3b0c816aca622e1"},"schema_version":"1.0"},"canonical_sha256":"fc3ad18e9583f81b850b3395dff610fed16f3876ffbfcfd93b4265a4686b42ab","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:22:04.817406Z","signature_b64":"MQj/ORQRjagW209TlfLEuvvcFIps20asLok9cnc5LHh+BAaVY9HmCoU2kDOiCl2smx6GimERkI37EGZkNz6/Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"fc3ad18e9583f81b850b3395dff610fed16f3876ffbfcfd93b4265a4686b42ab","last_reissued_at":"2026-07-04T16:22:04.817055Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:22:04.817055Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"nucl-th/0007052","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":"2026-07-04T16:22:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"93DESG2zEAAbm96g0sZCBTmzbkpPO4RmjzFlc21T2uZuVrlrgYJ0zOuVrfMfoon2BCwu+hbfYFC3UXwGS6YTAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T01:42:38.063225Z"},"content_sha256":"d97019c03037028f5dd449d1cad56657d0680ef5b62746c02fa1a8898d2b0e1b","schema_version":"1.0","event_id":"sha256:d97019c03037028f5dd449d1cad56657d0680ef5b62746c02fa1a8898d2b0e1b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2000:7Q5NDDUVQP4BXBILGOK575QQ73","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Coupling of Dipole Mode to gamma-unstable Quadrupole Oscillations","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Vitturi, C.E. Alonso, E.G. Lanza, J.M. Arias, M.V. Andres","submitted_at":"2000-07-24T12:28:54Z","abstract_excerpt":"The coupling of the high-lying dipole mode to the low-lying quadrupole modes for the case of deformed gamma-unstable nuclei is studied. Results from the geometrical model are compared to those obtained within the dipole boson model. Consistent results are obtained in both models. The dipole boson model is treated within the intrinsic frame, with subsequent projection onto the laboratory frame. As an application, calculations of photonuclear cross-sections in gamma-unstable nuclei are presented."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0007052","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/nucl-th/0007052/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:22:04Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5/2a9mk305j6VrIvTcHNgAmLV6/LYz3TzW1kRMos7+YiiDbQjg1MBaZTezL5SeEoTOK5wUn1n9qvIPLOpcBNCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-05T01:42:38.063615Z"},"content_sha256":"282196ce48a3742ec59639dc4d37a059acde6e0cca536be096365699c44a7d80","schema_version":"1.0","event_id":"sha256:282196ce48a3742ec59639dc4d37a059acde6e0cca536be096365699c44a7d80"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/7Q5NDDUVQP4BXBILGOK575QQ73/bundle.json","state_url":"https://pith.science/pith/7Q5NDDUVQP4BXBILGOK575QQ73/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/7Q5NDDUVQP4BXBILGOK575QQ73/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":"2026-07-05T01:42:38Z","links":{"resolver":"https://pith.science/pith/7Q5NDDUVQP4BXBILGOK575QQ73","bundle":"https://pith.science/pith/7Q5NDDUVQP4BXBILGOK575QQ73/bundle.json","state":"https://pith.science/pith/7Q5NDDUVQP4BXBILGOK575QQ73/state.json","well_known_bundle":"https://pith.science/.well-known/pith/7Q5NDDUVQP4BXBILGOK575QQ73/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2000:7Q5NDDUVQP4BXBILGOK575QQ73","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":"86786a5cfa0862809c2530b788fb2f53328e725dc62a3734b3b0c816aca622e1","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2000-07-24T12:28:54Z","title_canon_sha256":"3c98f0d749cb1c6d0a89d63f070ac57be49f102046575ce1d26f4e7ef98b4d1b"},"schema_version":"1.0","source":{"id":"nucl-th/0007052","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"nucl-th/0007052","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0007052v1","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0007052","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"pith_short_12","alias_value":"7Q5NDDUVQP4B","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"pith_short_16","alias_value":"7Q5NDDUVQP4BXBIL","created_at":"2026-07-04T16:22:04Z"},{"alias_kind":"pith_short_8","alias_value":"7Q5NDDUV","created_at":"2026-07-04T16:22:04Z"}],"graph_snapshots":[{"event_id":"sha256:282196ce48a3742ec59639dc4d37a059acde6e0cca536be096365699c44a7d80","target":"graph","created_at":"2026-07-04T16:22:04Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/nucl-th/0007052/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The coupling of the high-lying dipole mode to the low-lying quadrupole modes for the case of deformed gamma-unstable nuclei is studied. Results from the geometrical model are compared to those obtained within the dipole boson model. Consistent results are obtained in both models. The dipole boson model is treated within the intrinsic frame, with subsequent projection onto the laboratory frame. As an application, calculations of photonuclear cross-sections in gamma-unstable nuclei are presented.","authors_text":"A. Vitturi, C.E. Alonso, E.G. Lanza, J.M. Arias, M.V. Andres","cross_cats":[],"headline":"","license":"","primary_cat":"nucl-th","submitted_at":"2000-07-24T12:28:54Z","title":"Coupling of Dipole Mode to gamma-unstable Quadrupole Oscillations"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0007052","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:d97019c03037028f5dd449d1cad56657d0680ef5b62746c02fa1a8898d2b0e1b","target":"record","created_at":"2026-07-04T16:22:04Z","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":"86786a5cfa0862809c2530b788fb2f53328e725dc62a3734b3b0c816aca622e1","cross_cats_sorted":[],"license":"","primary_cat":"nucl-th","submitted_at":"2000-07-24T12:28:54Z","title_canon_sha256":"3c98f0d749cb1c6d0a89d63f070ac57be49f102046575ce1d26f4e7ef98b4d1b"},"schema_version":"1.0","source":{"id":"nucl-th/0007052","kind":"arxiv","version":1}},"canonical_sha256":"fc3ad18e9583f81b850b3395dff610fed16f3876ffbfcfd93b4265a4686b42ab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"fc3ad18e9583f81b850b3395dff610fed16f3876ffbfcfd93b4265a4686b42ab","first_computed_at":"2026-07-04T16:22:04.817055Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:22:04.817055Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"MQj/ORQRjagW209TlfLEuvvcFIps20asLok9cnc5LHh+BAaVY9HmCoU2kDOiCl2smx6GimERkI37EGZkNz6/Ag==","signature_status":"signed_v1","signed_at":"2026-07-04T16:22:04.817406Z","signed_message":"canonical_sha256_bytes"},"source_id":"nucl-th/0007052","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d97019c03037028f5dd449d1cad56657d0680ef5b62746c02fa1a8898d2b0e1b","sha256:282196ce48a3742ec59639dc4d37a059acde6e0cca536be096365699c44a7d80"],"state_sha256":"dae86e8118495f8a17aada2f6b68ca53defda776b99747f380a69997f213d3e7"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pS5bejE2v92mJLIaYqPwJSmrZQkJ/KjRKBFtTAlwcjrYCJ7AWnXKg340bP0PmOiPojBy18JKF5HdIoNxw57PAA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-05T01:42:38.065755Z","bundle_sha256":"54818376ad323f400267ef5a6929ff53ae57fb2e8724a86f1e3b043b2c33a842"}}