{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:5TVK2P4GVNZNTXIBPH6ONVCB4X","short_pith_number":"pith:5TVK2P4G","schema_version":"1.0","canonical_sha256":"eceaad3f86ab72d9dd0179fce6d441e5c434163223d1bb790e61bd41693df845","source":{"kind":"arxiv","id":"2305.09182","version":2},"attestation_state":"computed","paper":{"title":"Evidence of bicluster structure in the ground state of $^{20}$Ne","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"N. Itagaki, W. Horiuchi, Y. Yamaguchi","submitted_at":"2023-05-16T05:45:23Z","abstract_excerpt":"We explore the structure of the ground state of $^{20}$Ne by investigating various density profiles. Four candidates for the ground state configurations, (a) $j$-$j$ coupling and (b) SU(3) shell model and (c) $5\\alpha$ and (d) $^{16}{\\rm O}+\\alpha$ cluster model configurations are generated by utilizing the antisymmetrized quasicluster model. A high-energy reaction theory, the Glauber model, relates these one-body density distributions and reaction observables. The angular distributions of the elastic scattering cross sections clearly distinguish these configurations and tell which is the most"},"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":"2305.09182","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2023-05-16T05:45:23Z","cross_cats_sorted":[],"title_canon_sha256":"3bc2cf86c4befeace543ebe9dbe6888506bd514c140e6008e4a0ea1b8c46b4c3","abstract_canon_sha256":"e0ca840e4ef38f709ea0c3a8cc26aa00eae5f73df1805c9ccf2f406f6520c149"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:36:36.780558Z","signature_b64":"GNB2w1VWCK8X+U2UYNBoi7oZv3z1KWwjpMVPCSoojIrkD6yyda9AiIdI2tc5r2X+I55sDYYVfwfo1bJEDTEZCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"eceaad3f86ab72d9dd0179fce6d441e5c434163223d1bb790e61bd41693df845","last_reissued_at":"2026-07-05T06:36:36.780019Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:36:36.780019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evidence of bicluster structure in the ground state of $^{20}$Ne","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"N. Itagaki, W. Horiuchi, Y. Yamaguchi","submitted_at":"2023-05-16T05:45:23Z","abstract_excerpt":"We explore the structure of the ground state of $^{20}$Ne by investigating various density profiles. Four candidates for the ground state configurations, (a) $j$-$j$ coupling and (b) SU(3) shell model and (c) $5\\alpha$ and (d) $^{16}{\\rm O}+\\alpha$ cluster model configurations are generated by utilizing the antisymmetrized quasicluster model. A high-energy reaction theory, the Glauber model, relates these one-body density distributions and reaction observables. The angular distributions of the elastic scattering cross sections clearly distinguish these configurations and tell which is the most"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2305.09182","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2305.09182/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2305.09182","created_at":"2026-07-05T06:36:36.780080+00:00"},{"alias_kind":"arxiv_version","alias_value":"2305.09182v2","created_at":"2026-07-05T06:36:36.780080+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2305.09182","created_at":"2026-07-05T06:36:36.780080+00:00"},{"alias_kind":"pith_short_12","alias_value":"5TVK2P4GVNZN","created_at":"2026-07-05T06:36:36.780080+00:00"},{"alias_kind":"pith_short_16","alias_value":"5TVK2P4GVNZNTXIB","created_at":"2026-07-05T06:36:36.780080+00:00"},{"alias_kind":"pith_short_8","alias_value":"5TVK2P4G","created_at":"2026-07-05T06:36:36.780080+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.24079","citing_title":"Initial spin fluctuations as a probe of cluster spin structure in $^{16}\\mathrm{O}$ and $^{20}\\mathrm{Ne}$ nuclei","ref_index":65,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X","json":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X.json","graph_json":"https://pith.science/api/pith-number/5TVK2P4GVNZNTXIBPH6ONVCB4X/graph.json","events_json":"https://pith.science/api/pith-number/5TVK2P4GVNZNTXIBPH6ONVCB4X/events.json","paper":"https://pith.science/paper/5TVK2P4G"},"agent_actions":{"view_html":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X","download_json":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X.json","view_paper":"https://pith.science/paper/5TVK2P4G","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2305.09182&json=true","fetch_graph":"https://pith.science/api/pith-number/5TVK2P4GVNZNTXIBPH6ONVCB4X/graph.json","fetch_events":"https://pith.science/api/pith-number/5TVK2P4GVNZNTXIBPH6ONVCB4X/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X/action/storage_attestation","attest_author":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X/action/author_attestation","sign_citation":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X/action/citation_signature","submit_replication":"https://pith.science/pith/5TVK2P4GVNZNTXIBPH6ONVCB4X/action/replication_record"}},"created_at":"2026-07-05T06:36:36.780080+00:00","updated_at":"2026-07-05T06:36:36.780080+00:00"}