{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:4LLIFMQEQRZNZFQ5PMIIJ2XCVS","short_pith_number":"pith:4LLIFMQE","schema_version":"1.0","canonical_sha256":"e2d682b2048472dc961d7b1084eae2acbb442f19210b5188d0689ec6f0b03c17","source":{"kind":"arxiv","id":"1706.05514","version":1},"attestation_state":"computed","paper":{"title":"Formation and decay of resonance state in $^{9}$Be and $^{9}$B nuclei. Microscopic three-cluster model investigations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"K. Kat\\=o, N. Zh. Takibayev, V. S. Vasilevsky","submitted_at":"2017-06-17T11:21:37Z","abstract_excerpt":"We study nature of the low-lying resonance states in mirror nuclei $^{9}$Be and $^{9}$B. Investigations are performed within a three-cluster model. The model makes use of the hyperspherical harmonics, which provides convenient description of three-cluster continuum. The dominant three-cluster configurations $\\alpha+\\alpha+n$ and $\\alpha+\\alpha+p$ in $^{9}$Be and $^{9}$B, respectively, are taken into account. Dominant decay channels for all resonance states in $^{9}$Be and $^{9}$B are explored. Much attention is paid to the controversial $1/2^{+}$ resonance states in both nuclei. We study effec"},"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":"1706.05514","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2017-06-17T11:21:37Z","cross_cats_sorted":[],"title_canon_sha256":"2278cf611932af61a8ea135440811d1bf320559851bf64bca2c3efb8fdd9024c","abstract_canon_sha256":"32b88884373abf5d456cc549fe9ef4994e5eea685b65a7585c5c7816c888cb27"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:33:17.333692Z","signature_b64":"iIDiQghEv1IkQtvYbZfJJItMOk5H0m/GUJA6j0Nr3y6wWy99ajBe8Re4JRR5jIm+JFlTUSJtQelm3EwSzemyCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e2d682b2048472dc961d7b1084eae2acbb442f19210b5188d0689ec6f0b03c17","last_reissued_at":"2026-05-18T00:33:17.332977Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:33:17.332977Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Formation and decay of resonance state in $^{9}$Be and $^{9}$B nuclei. Microscopic three-cluster model investigations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"K. Kat\\=o, N. Zh. Takibayev, V. S. Vasilevsky","submitted_at":"2017-06-17T11:21:37Z","abstract_excerpt":"We study nature of the low-lying resonance states in mirror nuclei $^{9}$Be and $^{9}$B. Investigations are performed within a three-cluster model. The model makes use of the hyperspherical harmonics, which provides convenient description of three-cluster continuum. The dominant three-cluster configurations $\\alpha+\\alpha+n$ and $\\alpha+\\alpha+p$ in $^{9}$Be and $^{9}$B, respectively, are taken into account. Dominant decay channels for all resonance states in $^{9}$Be and $^{9}$B are explored. Much attention is paid to the controversial $1/2^{+}$ resonance states in both nuclei. We study effec"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1706.05514","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":"1706.05514","created_at":"2026-05-18T00:33:17.333096+00:00"},{"alias_kind":"arxiv_version","alias_value":"1706.05514v1","created_at":"2026-05-18T00:33:17.333096+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1706.05514","created_at":"2026-05-18T00:33:17.333096+00:00"},{"alias_kind":"pith_short_12","alias_value":"4LLIFMQEQRZN","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_16","alias_value":"4LLIFMQEQRZNZFQ5","created_at":"2026-05-18T12:31:00.734936+00:00"},{"alias_kind":"pith_short_8","alias_value":"4LLIFMQE","created_at":"2026-05-18T12:31:00.734936+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/4LLIFMQEQRZNZFQ5PMIIJ2XCVS","json":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS.json","graph_json":"https://pith.science/api/pith-number/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/graph.json","events_json":"https://pith.science/api/pith-number/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/events.json","paper":"https://pith.science/paper/4LLIFMQE"},"agent_actions":{"view_html":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS","download_json":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS.json","view_paper":"https://pith.science/paper/4LLIFMQE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1706.05514&json=true","fetch_graph":"https://pith.science/api/pith-number/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/graph.json","fetch_events":"https://pith.science/api/pith-number/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/action/storage_attestation","attest_author":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/action/author_attestation","sign_citation":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/action/citation_signature","submit_replication":"https://pith.science/pith/4LLIFMQEQRZNZFQ5PMIIJ2XCVS/action/replication_record"}},"created_at":"2026-05-18T00:33:17.333096+00:00","updated_at":"2026-05-18T00:33:17.333096+00:00"}