{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:7DOYKQ335TIYC2WSSGCO5HXAGW","short_pith_number":"pith:7DOYKQ33","schema_version":"1.0","canonical_sha256":"f8dd85437becd1816ad29184ee9ee0358027c59d401d36e37de109d6f650f8dd","source":{"kind":"arxiv","id":"1402.6102","version":1},"attestation_state":"computed","paper":{"title":"Microscopic description of octupole shape-phase transitions in light actinides and rare-earth nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Bing-Nan Lu, D. Vretenar, K. Nomura, T. Niksic","submitted_at":"2014-02-25T09:29:35Z","abstract_excerpt":"A systematic analysis of low-lying quadrupole and octupole collective states is presented, based on the microscopic energy density functional framework. By mapping the deformation constrained self-consistent axially symmetric mean-field energy surfaces onto the equivalent Hamiltonian of the $sdf$ interacting boson model (IBM), that is, onto the energy expectation value in the boson condensate state, the Hamiltonian parameters are determined. The study is based on the global relativistic energy density functional DD-PC1. The resulting IBM Hamiltonian is used to calculate excitation spectra and "},"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":"1402.6102","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-02-25T09:29:35Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"aac7d6550dceeec95adeea30d44cd867a2fbcce469ce61ab1bb61ab9e7492039","abstract_canon_sha256":"358e12346a71bde075377df52a31ba5bfae1222d8049158d6845a8d5d999b0d6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:57:51.624463Z","signature_b64":"H/MjogzLP84sLwYC4TNjfJg/fGzO3/9d4j7ehT+ap5fRIGUgZ0C8JtT1M2No6WgEL6dCDFh6gcV5FIwlOlVGDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f8dd85437becd1816ad29184ee9ee0358027c59d401d36e37de109d6f650f8dd","last_reissued_at":"2026-05-18T02:57:51.623997Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:57:51.623997Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Microscopic description of octupole shape-phase transitions in light actinides and rare-earth nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"Bing-Nan Lu, D. Vretenar, K. Nomura, T. Niksic","submitted_at":"2014-02-25T09:29:35Z","abstract_excerpt":"A systematic analysis of low-lying quadrupole and octupole collective states is presented, based on the microscopic energy density functional framework. By mapping the deformation constrained self-consistent axially symmetric mean-field energy surfaces onto the equivalent Hamiltonian of the $sdf$ interacting boson model (IBM), that is, onto the energy expectation value in the boson condensate state, the Hamiltonian parameters are determined. The study is based on the global relativistic energy density functional DD-PC1. The resulting IBM Hamiltonian is used to calculate excitation spectra and "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1402.6102","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":"1402.6102","created_at":"2026-05-18T02:57:51.624065+00:00"},{"alias_kind":"arxiv_version","alias_value":"1402.6102v1","created_at":"2026-05-18T02:57:51.624065+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1402.6102","created_at":"2026-05-18T02:57:51.624065+00:00"},{"alias_kind":"pith_short_12","alias_value":"7DOYKQ335TIY","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_16","alias_value":"7DOYKQ335TIYC2WS","created_at":"2026-05-18T12:28:16.859392+00:00"},{"alias_kind":"pith_short_8","alias_value":"7DOYKQ33","created_at":"2026-05-18T12:28:16.859392+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/7DOYKQ335TIYC2WSSGCO5HXAGW","json":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW.json","graph_json":"https://pith.science/api/pith-number/7DOYKQ335TIYC2WSSGCO5HXAGW/graph.json","events_json":"https://pith.science/api/pith-number/7DOYKQ335TIYC2WSSGCO5HXAGW/events.json","paper":"https://pith.science/paper/7DOYKQ33"},"agent_actions":{"view_html":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW","download_json":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW.json","view_paper":"https://pith.science/paper/7DOYKQ33","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1402.6102&json=true","fetch_graph":"https://pith.science/api/pith-number/7DOYKQ335TIYC2WSSGCO5HXAGW/graph.json","fetch_events":"https://pith.science/api/pith-number/7DOYKQ335TIYC2WSSGCO5HXAGW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW/action/storage_attestation","attest_author":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW/action/author_attestation","sign_citation":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW/action/citation_signature","submit_replication":"https://pith.science/pith/7DOYKQ335TIYC2WSSGCO5HXAGW/action/replication_record"}},"created_at":"2026-05-18T02:57:51.624065+00:00","updated_at":"2026-05-18T02:57:51.624065+00:00"}