{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:ZAHW5D63LVCU7DA2TOWMIYAY2B","short_pith_number":"pith:ZAHW5D63","schema_version":"1.0","canonical_sha256":"c80f6e8fdb5d454f8c1a9bacc46018d0503f089294e855c525897d24af159429","source":{"kind":"arxiv","id":"1809.05899","version":1},"attestation_state":"computed","paper":{"title":"Shape Coexistence and Mixing of Low-Lying $0^+$ States in $^{96}$Sr","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A.B. Garnsworthy, A. Cheeseman, A. Chester, A. Knapton, A. Matta, A. Sanetullaev, C.Aa. Diget, C. Andreoiu, C.E. Svensson, C.S. Bancroft, C. Unsworth, D. Miller, D.S. Cross, F. Ames, G. Hackman, J. Lassen, K. Kuhn, K. Wimmer, M. Marchetto, M. Moukaddam, N.A. Orr, N. Sachmpazidi, N. Terpstra, P.C. Bender, P.J. Voss, R.A.E. Austin, R. Braid, R. Kanungo, R. Kr\\\"ucken, R. Laxdal, S. Cruz, T. Bruhn, T. Drake, W. Korten, W.N. Catford","submitted_at":"2018-09-16T15:47:36Z","abstract_excerpt":"The low energy excited $0_{2,3}^+$ states in $^{96}$Sr are amongst the most prominent examples of shape coexistence across the nuclear landscape. In this work, the neutron $[2s_{1/2}]^2$ content of the $0_{1,2,3}^+$ states in $^{96}$Sr was determined by means of the d($^{95}$Sr,p) transfer reaction at the TRIUMF-ISAC2 facility using the SHARC and TIGRESS arrays. Spectroscopic factors of 0.19(3) and 0.22(3) were extracted for the $^{96}$Sr ground and 1229~keV $0^+$ states, respectively, by fitting the experimental angular distributions to DWBA reaction model calculations. A detailed analysis of"},"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":"1809.05899","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2018-09-16T15:47:36Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"98d99f75a02ba6ee8f727ab3c15363fce8bb0016cb2e5a63747801cd8b23d20c","abstract_canon_sha256":"edf49be76501adc9a8c00f8ffded78c06bc15a352fd56f9fdd777f0b94a21770"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:03:01.437460Z","signature_b64":"pXvGfdJ+tuO2uj7OeKDxE2Ked3ZAnvnxks1v4U8ACwbhB56h1343vWAwMyWcMjs7+zXpTGV0Bpgqyczqc1z0AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c80f6e8fdb5d454f8c1a9bacc46018d0503f089294e855c525897d24af159429","last_reissued_at":"2026-05-18T00:03:01.436979Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:03:01.436979Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Shape Coexistence and Mixing of Low-Lying $0^+$ States in $^{96}$Sr","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A.B. Garnsworthy, A. Cheeseman, A. Chester, A. Knapton, A. Matta, A. Sanetullaev, C.Aa. Diget, C. Andreoiu, C.E. Svensson, C.S. Bancroft, C. Unsworth, D. Miller, D.S. Cross, F. Ames, G. Hackman, J. Lassen, K. Kuhn, K. Wimmer, M. Marchetto, M. Moukaddam, N.A. Orr, N. Sachmpazidi, N. Terpstra, P.C. Bender, P.J. Voss, R.A.E. Austin, R. Braid, R. Kanungo, R. Kr\\\"ucken, R. Laxdal, S. Cruz, T. Bruhn, T. Drake, W. Korten, W.N. Catford","submitted_at":"2018-09-16T15:47:36Z","abstract_excerpt":"The low energy excited $0_{2,3}^+$ states in $^{96}$Sr are amongst the most prominent examples of shape coexistence across the nuclear landscape. In this work, the neutron $[2s_{1/2}]^2$ content of the $0_{1,2,3}^+$ states in $^{96}$Sr was determined by means of the d($^{95}$Sr,p) transfer reaction at the TRIUMF-ISAC2 facility using the SHARC and TIGRESS arrays. Spectroscopic factors of 0.19(3) and 0.22(3) were extracted for the $^{96}$Sr ground and 1229~keV $0^+$ states, respectively, by fitting the experimental angular distributions to DWBA reaction model calculations. A detailed analysis of"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.05899","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":"1809.05899","created_at":"2026-05-18T00:03:01.437049+00:00"},{"alias_kind":"arxiv_version","alias_value":"1809.05899v1","created_at":"2026-05-18T00:03:01.437049+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.05899","created_at":"2026-05-18T00:03:01.437049+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZAHW5D63LVCU","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZAHW5D63LVCU7DA2","created_at":"2026-05-18T12:33:04.347982+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZAHW5D63","created_at":"2026-05-18T12:33:04.347982+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/ZAHW5D63LVCU7DA2TOWMIYAY2B","json":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B.json","graph_json":"https://pith.science/api/pith-number/ZAHW5D63LVCU7DA2TOWMIYAY2B/graph.json","events_json":"https://pith.science/api/pith-number/ZAHW5D63LVCU7DA2TOWMIYAY2B/events.json","paper":"https://pith.science/paper/ZAHW5D63"},"agent_actions":{"view_html":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B","download_json":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B.json","view_paper":"https://pith.science/paper/ZAHW5D63","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1809.05899&json=true","fetch_graph":"https://pith.science/api/pith-number/ZAHW5D63LVCU7DA2TOWMIYAY2B/graph.json","fetch_events":"https://pith.science/api/pith-number/ZAHW5D63LVCU7DA2TOWMIYAY2B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B/action/storage_attestation","attest_author":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B/action/author_attestation","sign_citation":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B/action/citation_signature","submit_replication":"https://pith.science/pith/ZAHW5D63LVCU7DA2TOWMIYAY2B/action/replication_record"}},"created_at":"2026-05-18T00:03:01.437049+00:00","updated_at":"2026-05-18T00:03:01.437049+00:00"}