{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:A7SNWIV5EC6BU33KU55LDMRJWW","short_pith_number":"pith:A7SNWIV5","schema_version":"1.0","canonical_sha256":"07e4db22bd20bc1a6f6aa77ab1b229b5a7f07c75bad9a9e6c892165d614a944e","source":{"kind":"arxiv","id":"1403.4812","version":2},"attestation_state":"computed","paper":{"title":"A microscopic benchmark-study of triaxiality in low-lying states of 76Kr","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"J. Meng, J. M. Yao, K. Hagino, P. Ring, Z. P. Li","submitted_at":"2014-03-19T14:21:37Z","abstract_excerpt":"We report on a seven-dimensional generator coordinate calculation in the two deformation parameters $\\beta$ and $\\gamma$ together with projection on three-dimensional angular momentum and two particle numbers for the low-lying states in $^{76}$Kr. These calculations are based on covariant density functional theory. Excellent agreement is found with the data for the spectrum and the electric multipole transition strengths. This answers the important question of dynamic correlations and triaxiality in a fully microscopic way. We find that triaxial configurations dominate both the ground state an"},"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":"1403.4812","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-03-19T14:21:37Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"e8df3b02590ba38c67d03e4f70f680ced1872918b257d0ab8cc4a7bea1083d4d","abstract_canon_sha256":"6fe3ca6b3030fae7cadf50871657803e3cf6434a2ede37d0516f7330242cba31"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:52:33.804385Z","signature_b64":"lFhmYAmL6PsLkkc5QhWyJLGZGriQpFY5kKqsM7FajKW8kSHxJX07mxvsn4KCwn49OYjt/ZXW2/mNUtsjZcrYDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"07e4db22bd20bc1a6f6aa77ab1b229b5a7f07c75bad9a9e6c892165d614a944e","last_reissued_at":"2026-05-18T02:52:33.803895Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:52:33.803895Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A microscopic benchmark-study of triaxiality in low-lying states of 76Kr","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"J. Meng, J. M. Yao, K. Hagino, P. Ring, Z. P. Li","submitted_at":"2014-03-19T14:21:37Z","abstract_excerpt":"We report on a seven-dimensional generator coordinate calculation in the two deformation parameters $\\beta$ and $\\gamma$ together with projection on three-dimensional angular momentum and two particle numbers for the low-lying states in $^{76}$Kr. These calculations are based on covariant density functional theory. Excellent agreement is found with the data for the spectrum and the electric multipole transition strengths. This answers the important question of dynamic correlations and triaxiality in a fully microscopic way. We find that triaxial configurations dominate both the ground state an"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1403.4812","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":""},"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":"1403.4812","created_at":"2026-05-18T02:52:33.803965+00:00"},{"alias_kind":"arxiv_version","alias_value":"1403.4812v2","created_at":"2026-05-18T02:52:33.803965+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1403.4812","created_at":"2026-05-18T02:52:33.803965+00:00"},{"alias_kind":"pith_short_12","alias_value":"A7SNWIV5EC6B","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_16","alias_value":"A7SNWIV5EC6BU33K","created_at":"2026-05-18T12:28:19.803747+00:00"},{"alias_kind":"pith_short_8","alias_value":"A7SNWIV5","created_at":"2026-05-18T12:28:19.803747+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.11244","citing_title":"Multireference covariant density functional theory for shape coexistence and isomerism in $^{43}$S","ref_index":38,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW","json":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW.json","graph_json":"https://pith.science/api/pith-number/A7SNWIV5EC6BU33KU55LDMRJWW/graph.json","events_json":"https://pith.science/api/pith-number/A7SNWIV5EC6BU33KU55LDMRJWW/events.json","paper":"https://pith.science/paper/A7SNWIV5"},"agent_actions":{"view_html":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW","download_json":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW.json","view_paper":"https://pith.science/paper/A7SNWIV5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1403.4812&json=true","fetch_graph":"https://pith.science/api/pith-number/A7SNWIV5EC6BU33KU55LDMRJWW/graph.json","fetch_events":"https://pith.science/api/pith-number/A7SNWIV5EC6BU33KU55LDMRJWW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW/action/storage_attestation","attest_author":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW/action/author_attestation","sign_citation":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW/action/citation_signature","submit_replication":"https://pith.science/pith/A7SNWIV5EC6BU33KU55LDMRJWW/action/replication_record"}},"created_at":"2026-05-18T02:52:33.803965+00:00","updated_at":"2026-05-18T02:52:33.803965+00:00"}