{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:TAY74SIL3FTC4UAV3QBZLFX5HL","short_pith_number":"pith:TAY74SIL","schema_version":"1.0","canonical_sha256":"9831fe490bd9662e5015dc039596fd3ac7c7a96185c7efd579d7fb34b46e54ce","source":{"kind":"arxiv","id":"0804.4743","version":2},"attestation_state":"computed","paper":{"title":"Mass Measurements and Implications for the Energy of the High-Spin Isomer in 94Ag","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Jokinen, A. Kankainen, A. Popov, A. Saastamoinen, C. Weber, D.M. Seliverstov, G. Vorobjev, H. Penttil\\\"a, I.D. Moore, J. \\\"Ayst\\\"o, J. Hakala, J. Rissanen, L. Batist, S. Eliseev, S. Rahaman, S. Rinta-Antila, T. Eronen, T. Sonoda, U. Hager, V.-V. Elomaa, Yu.N. Novikov","submitted_at":"2008-04-30T06:27:06Z","abstract_excerpt":"Nuclides in the vicinity of 94Ag have been studied with the Penning trap mass spectrometer JYFLTRAP at the Ion-Guide Separator On-Line. The masses of the two-proton-decay daughter 92Rh and the beta-decay daughter 94Pd of the high-spin isomer in 94Ag have been measured, and the masses of 93Pd and 94Ag have been deduced. When combined with the data from the one-proton or two-proton-decay experiments, the results lead to contradictory mass excess values for the high-spin isomer in 94Ag, -46370(170) or -44970(100) keV, corresponding to excitation energies of 6960(400) or 8360(370) keV, respectivel"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"0804.4743","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2008-04-30T06:27:06Z","cross_cats_sorted":[],"title_canon_sha256":"80da9a4227609dafdcc48459329e1bc48fbab5697a5526f288ac5f86dcbb7406","abstract_canon_sha256":"808283556e4bdb8ed4129c6f2f97e5045bc4a8b6b02093463e7ddb1766c4014e"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:30:05.834665Z","signature_b64":"IPOl9Gt3CxEFn28sZ+DUgPXLdqg2lZP/DwRoKmKFDvQVMBthsrbT1S849n0CZ1LDk316EfXxmKeui7vWxeRABQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9831fe490bd9662e5015dc039596fd3ac7c7a96185c7efd579d7fb34b46e54ce","last_reissued_at":"2026-07-04T15:30:05.834223Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:30:05.834223Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mass Measurements and Implications for the Energy of the High-Spin Isomer in 94Ag","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. Jokinen, A. Kankainen, A. Popov, A. Saastamoinen, C. Weber, D.M. Seliverstov, G. Vorobjev, H. Penttil\\\"a, I.D. Moore, J. \\\"Ayst\\\"o, J. Hakala, J. Rissanen, L. Batist, S. Eliseev, S. Rahaman, S. Rinta-Antila, T. Eronen, T. Sonoda, U. Hager, V.-V. Elomaa, Yu.N. Novikov","submitted_at":"2008-04-30T06:27:06Z","abstract_excerpt":"Nuclides in the vicinity of 94Ag have been studied with the Penning trap mass spectrometer JYFLTRAP at the Ion-Guide Separator On-Line. The masses of the two-proton-decay daughter 92Rh and the beta-decay daughter 94Pd of the high-spin isomer in 94Ag have been measured, and the masses of 93Pd and 94Ag have been deduced. When combined with the data from the one-proton or two-proton-decay experiments, the results lead to contradictory mass excess values for the high-spin isomer in 94Ag, -46370(170) or -44970(100) keV, corresponding to excitation energies of 6960(400) or 8360(370) keV, respectivel"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0804.4743","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/0804.4743/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"},"aliases":[{"alias_kind":"arxiv","alias_value":"0804.4743","created_at":"2026-07-04T15:30:05.834292+00:00"},{"alias_kind":"arxiv_version","alias_value":"0804.4743v2","created_at":"2026-07-04T15:30:05.834292+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0804.4743","created_at":"2026-07-04T15:30:05.834292+00:00"},{"alias_kind":"pith_short_12","alias_value":"TAY74SIL3FTC","created_at":"2026-07-04T15:30:05.834292+00:00"},{"alias_kind":"pith_short_16","alias_value":"TAY74SIL3FTC4UAV","created_at":"2026-07-04T15:30:05.834292+00:00"},{"alias_kind":"pith_short_8","alias_value":"TAY74SIL","created_at":"2026-07-04T15:30:05.834292+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL","json":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL.json","graph_json":"https://pith.science/api/pith-number/TAY74SIL3FTC4UAV3QBZLFX5HL/graph.json","events_json":"https://pith.science/api/pith-number/TAY74SIL3FTC4UAV3QBZLFX5HL/events.json","paper":"https://pith.science/paper/TAY74SIL"},"agent_actions":{"view_html":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL","download_json":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL.json","view_paper":"https://pith.science/paper/TAY74SIL","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0804.4743&json=true","fetch_graph":"https://pith.science/api/pith-number/TAY74SIL3FTC4UAV3QBZLFX5HL/graph.json","fetch_events":"https://pith.science/api/pith-number/TAY74SIL3FTC4UAV3QBZLFX5HL/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL/action/storage_attestation","attest_author":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL/action/author_attestation","sign_citation":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL/action/citation_signature","submit_replication":"https://pith.science/pith/TAY74SIL3FTC4UAV3QBZLFX5HL/action/replication_record"}},"created_at":"2026-07-04T15:30:05.834292+00:00","updated_at":"2026-07-04T15:30:05.834292+00:00"}