{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:ZNZV2RUGWN3OV72HDG4J4V6JRC","short_pith_number":"pith:ZNZV2RUG","schema_version":"1.0","canonical_sha256":"cb735d4686b376eaff4719b89e57c988b68254880f7dbaebe90667666f915186","source":{"kind":"arxiv","id":"1603.07483","version":2},"attestation_state":"computed","paper":{"title":"Three-body model for an isoscalar spin-triplet neutron-proton pair in $^{102}{\\rm Sb}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Hiroyuki Sagawa, Yusuke Tanimura","submitted_at":"2016-03-24T08:59:35Z","abstract_excerpt":"We discuss the isoscalar $T=0, S=1$ pairing correlation in the low-lying states of $^{102}{\\rm Sb}={}^{100}{\\rm Sn}+p+n$ nucleus. To this end, we employ ${\\rm core}+p+n$ three-body model with the model space constructed by self-consistent mean-field calculations. The model is developed with both non-relativistic and relativistic effective interactions, the latter of which are found to be more realistic for the present case due to the pseudo-spin symmetry. It turns out that the $(L,S,T)=(0,1,0)$ pairing scheme is strongly hindered in $^{102}$Sb with the relativistic model because of the near de"},"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":"1603.07483","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-03-24T08:59:35Z","cross_cats_sorted":[],"title_canon_sha256":"9b3fae4b02c0914c453aa8e4d0aa36ed32348fe3953f4a57030f249aa808c7ee","abstract_canon_sha256":"d8235a8668d6ca56164041904052996491038a569dd3c1f74ed354c9ec2f1a31"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:10:50.146254Z","signature_b64":"Xqmb1+nxcGsQPTHyDJquN9WAtsvdQ5/dtN/I00xjmBdYFnOoFQU5IHh/nOFNVZ3pEVfFcR6IDLB3DjS4P1FtCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cb735d4686b376eaff4719b89e57c988b68254880f7dbaebe90667666f915186","last_reissued_at":"2026-05-18T01:10:50.145721Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:10:50.145721Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Three-body model for an isoscalar spin-triplet neutron-proton pair in $^{102}{\\rm Sb}$","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Hiroyuki Sagawa, Yusuke Tanimura","submitted_at":"2016-03-24T08:59:35Z","abstract_excerpt":"We discuss the isoscalar $T=0, S=1$ pairing correlation in the low-lying states of $^{102}{\\rm Sb}={}^{100}{\\rm Sn}+p+n$ nucleus. To this end, we employ ${\\rm core}+p+n$ three-body model with the model space constructed by self-consistent mean-field calculations. The model is developed with both non-relativistic and relativistic effective interactions, the latter of which are found to be more realistic for the present case due to the pseudo-spin symmetry. It turns out that the $(L,S,T)=(0,1,0)$ pairing scheme is strongly hindered in $^{102}$Sb with the relativistic model because of the near de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1603.07483","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":"1603.07483","created_at":"2026-05-18T01:10:50.145800+00:00"},{"alias_kind":"arxiv_version","alias_value":"1603.07483v2","created_at":"2026-05-18T01:10:50.145800+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1603.07483","created_at":"2026-05-18T01:10:50.145800+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZNZV2RUGWN3O","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZNZV2RUGWN3OV72H","created_at":"2026-05-18T12:30:55.937587+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZNZV2RUG","created_at":"2026-05-18T12:30:55.937587+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/ZNZV2RUGWN3OV72HDG4J4V6JRC","json":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC.json","graph_json":"https://pith.science/api/pith-number/ZNZV2RUGWN3OV72HDG4J4V6JRC/graph.json","events_json":"https://pith.science/api/pith-number/ZNZV2RUGWN3OV72HDG4J4V6JRC/events.json","paper":"https://pith.science/paper/ZNZV2RUG"},"agent_actions":{"view_html":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC","download_json":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC.json","view_paper":"https://pith.science/paper/ZNZV2RUG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1603.07483&json=true","fetch_graph":"https://pith.science/api/pith-number/ZNZV2RUGWN3OV72HDG4J4V6JRC/graph.json","fetch_events":"https://pith.science/api/pith-number/ZNZV2RUGWN3OV72HDG4J4V6JRC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC/action/storage_attestation","attest_author":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC/action/author_attestation","sign_citation":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC/action/citation_signature","submit_replication":"https://pith.science/pith/ZNZV2RUGWN3OV72HDG4J4V6JRC/action/replication_record"}},"created_at":"2026-05-18T01:10:50.145800+00:00","updated_at":"2026-05-18T01:10:50.145800+00:00"}