{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:RWIV3OJ3L6PVWCRRTHQQ7WJ7XD","short_pith_number":"pith:RWIV3OJ3","schema_version":"1.0","canonical_sha256":"8d915db93b5f9f5b0a3199e10fd93fb8d5cee5653e5ea6dab27c6734e0448643","source":{"kind":"arxiv","id":"1605.03784","version":1},"attestation_state":"computed","paper":{"title":"In-beam spectroscopy of medium- and high-spin states in $^{133}$Ce","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. D. Ayangeakaa, B. K. Nayak, C. J. Chiara, C. M. Petrache, D. Patel, D. Seweryniak, F. G. Kondev, J. T. Matta, M. P. Carpenter, P. W. Zhao, R. Palit, R. V. F. Janssens, S. Guo, S. S. Ghugre, S. Zhu, T. Lauritsen, U. Garg","submitted_at":"2016-05-12T12:38:46Z","abstract_excerpt":"Medium and high-spin states in $^{133}$Ce were investigated using the $^{116}$Cd($^{22}$Ne, $5n$) reaction and the Gammasphere array. The level scheme was extended up to an excitation energy of $\\sim22.8$ MeV and spin 93/2 . Eleven bands of quadrupole transitions and two new dipole bands are identified. The connections to low-lying states of the previously known, high-spin triaxial bands were firmly established, thus fixing the excitation energy and, in many cases, the spin parity of the levels. Based on comparisons with cranked Nilsson-Strutinsky calculations and tilted axis cranking covarian"},"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":"1605.03784","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2016-05-12T12:38:46Z","cross_cats_sorted":[],"title_canon_sha256":"ff9ba8db9d6bddd4c2667e781afabb69791049fde53e08b33eeb104a000aae03","abstract_canon_sha256":"0a33d340f7892c4ee450228fe358b8761eb69210dd0af1c4b1c1b2501a7f9f29"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:13:46.936974Z","signature_b64":"FGPg26wvz8vm/nZMuDsVwMGg3L8hmlYuYIWHBbh6gBZ3AXiY4W8nBCZYXg3Bjc70FSqehRj5plJb5FO0i+ufBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d915db93b5f9f5b0a3199e10fd93fb8d5cee5653e5ea6dab27c6734e0448643","last_reissued_at":"2026-05-18T01:13:46.936200Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:13:46.936200Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"In-beam spectroscopy of medium- and high-spin states in $^{133}$Ce","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-ex","authors_text":"A. D. Ayangeakaa, B. K. Nayak, C. J. Chiara, C. M. Petrache, D. Patel, D. Seweryniak, F. G. Kondev, J. T. Matta, M. P. Carpenter, P. W. Zhao, R. Palit, R. V. F. Janssens, S. Guo, S. S. Ghugre, S. Zhu, T. Lauritsen, U. Garg","submitted_at":"2016-05-12T12:38:46Z","abstract_excerpt":"Medium and high-spin states in $^{133}$Ce were investigated using the $^{116}$Cd($^{22}$Ne, $5n$) reaction and the Gammasphere array. The level scheme was extended up to an excitation energy of $\\sim22.8$ MeV and spin 93/2 . Eleven bands of quadrupole transitions and two new dipole bands are identified. The connections to low-lying states of the previously known, high-spin triaxial bands were firmly established, thus fixing the excitation energy and, in many cases, the spin parity of the levels. Based on comparisons with cranked Nilsson-Strutinsky calculations and tilted axis cranking covarian"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1605.03784","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":"1605.03784","created_at":"2026-05-18T01:13:46.936332+00:00"},{"alias_kind":"arxiv_version","alias_value":"1605.03784v1","created_at":"2026-05-18T01:13:46.936332+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1605.03784","created_at":"2026-05-18T01:13:46.936332+00:00"},{"alias_kind":"pith_short_12","alias_value":"RWIV3OJ3L6PV","created_at":"2026-05-18T12:30:41.710351+00:00"},{"alias_kind":"pith_short_16","alias_value":"RWIV3OJ3L6PVWCRR","created_at":"2026-05-18T12:30:41.710351+00:00"},{"alias_kind":"pith_short_8","alias_value":"RWIV3OJ3","created_at":"2026-05-18T12:30:41.710351+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/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD","json":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD.json","graph_json":"https://pith.science/api/pith-number/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/graph.json","events_json":"https://pith.science/api/pith-number/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/events.json","paper":"https://pith.science/paper/RWIV3OJ3"},"agent_actions":{"view_html":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD","download_json":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD.json","view_paper":"https://pith.science/paper/RWIV3OJ3","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1605.03784&json=true","fetch_graph":"https://pith.science/api/pith-number/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/graph.json","fetch_events":"https://pith.science/api/pith-number/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/action/storage_attestation","attest_author":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/action/author_attestation","sign_citation":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/action/citation_signature","submit_replication":"https://pith.science/pith/RWIV3OJ3L6PVWCRRTHQQ7WJ7XD/action/replication_record"}},"created_at":"2026-05-18T01:13:46.936332+00:00","updated_at":"2026-05-18T01:13:46.936332+00:00"}