{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:TUBICALE7ANZF3DSEV277JSXU6","short_pith_number":"pith:TUBICALE","schema_version":"1.0","canonical_sha256":"9d02810164f81b92ec722575ffa657a78491df07758cb772db64ea19eca0fb95","source":{"kind":"arxiv","id":"1009.2691","version":1},"attestation_state":"computed","paper":{"title":"Low energy shape oscillations of negative parity in the main and shape-isomeric minima in actinides","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Skalski, M. Kowal","submitted_at":"2010-09-14T15:23:34Z","abstract_excerpt":"We study low energy shape oscillations of negative parity in the first and second (isomeric) minima in actinides. As a main tool we use the phenomenological Woods-Saxon potential with a variety of shape deformations. This allows to include a mixing of various multipolarities when considering oscillations with a fixed $K$ quantum number. The phonon energies are determined either from the collective Hamiltonian with the microscopic-macrocopic energy and cranking mass parameters, or from its simplified version with the constant mass parameters. The results for $K^{\\pi}=0^-$,$1^-$ in the first min"},"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":"1009.2691","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2010-09-14T15:23:34Z","cross_cats_sorted":[],"title_canon_sha256":"0b2c1bf5b0e3afafdfb32913f88edfc2c7237501ba6e9ddbfcde0b214ce18b6c","abstract_canon_sha256":"2db595e7a76e3a8e0f06eb74d0a9eb191bf55834f668e61818c67fb9bbc6cf3f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:35:36.387573Z","signature_b64":"/NLn7TQU+x3Cg7CRcCrIzeDQzMU8+St0+VmEQROVWSgTS8Zx34QbBh/84Oz8ykBLSep8VM1JiCVfKHuLVYPbBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9d02810164f81b92ec722575ffa657a78491df07758cb772db64ea19eca0fb95","last_reissued_at":"2026-05-18T04:35:36.386923Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:35:36.386923Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Low energy shape oscillations of negative parity in the main and shape-isomeric minima in actinides","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"J. Skalski, M. Kowal","submitted_at":"2010-09-14T15:23:34Z","abstract_excerpt":"We study low energy shape oscillations of negative parity in the first and second (isomeric) minima in actinides. As a main tool we use the phenomenological Woods-Saxon potential with a variety of shape deformations. This allows to include a mixing of various multipolarities when considering oscillations with a fixed $K$ quantum number. The phonon energies are determined either from the collective Hamiltonian with the microscopic-macrocopic energy and cranking mass parameters, or from its simplified version with the constant mass parameters. The results for $K^{\\pi}=0^-$,$1^-$ in the first min"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.2691","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1009.2691","created_at":"2026-05-18T04:35:36.387031+00:00"},{"alias_kind":"arxiv_version","alias_value":"1009.2691v1","created_at":"2026-05-18T04:35:36.387031+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.2691","created_at":"2026-05-18T04:35:36.387031+00:00"},{"alias_kind":"pith_short_12","alias_value":"TUBICALE7ANZ","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_16","alias_value":"TUBICALE7ANZF3DS","created_at":"2026-05-18T12:26:15.391820+00:00"},{"alias_kind":"pith_short_8","alias_value":"TUBICALE","created_at":"2026-05-18T12:26:15.391820+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/TUBICALE7ANZF3DSEV277JSXU6","json":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6.json","graph_json":"https://pith.science/api/pith-number/TUBICALE7ANZF3DSEV277JSXU6/graph.json","events_json":"https://pith.science/api/pith-number/TUBICALE7ANZF3DSEV277JSXU6/events.json","paper":"https://pith.science/paper/TUBICALE"},"agent_actions":{"view_html":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6","download_json":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6.json","view_paper":"https://pith.science/paper/TUBICALE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1009.2691&json=true","fetch_graph":"https://pith.science/api/pith-number/TUBICALE7ANZF3DSEV277JSXU6/graph.json","fetch_events":"https://pith.science/api/pith-number/TUBICALE7ANZF3DSEV277JSXU6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6/action/storage_attestation","attest_author":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6/action/author_attestation","sign_citation":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6/action/citation_signature","submit_replication":"https://pith.science/pith/TUBICALE7ANZF3DSEV277JSXU6/action/replication_record"}},"created_at":"2026-05-18T04:35:36.387031+00:00","updated_at":"2026-05-18T04:35:36.387031+00:00"}