{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:BVECGYLRJUWVHEABY6JOKLS7PZ","short_pith_number":"pith:BVECGYLR","schema_version":"1.0","canonical_sha256":"0d482361714d2d539001c792e52e5f7e63d31f3e4324d4f9a58170384d73c263","source":{"kind":"arxiv","id":"1201.2497","version":1},"attestation_state":"computed","paper":{"title":"Deformation of Ne isotopes in the island-of-inversion region","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Kazuyuki Ogata, Kosho Minomo, Masaaki Kimura, Masanobu Yahiro, Shingo Tagami, Takenori Sumi, Takuma Matsumoto, Yoshifumi R. Shimizu","submitted_at":"2012-01-12T08:16:59Z","abstract_excerpt":"The deformation of Ne isotopes in the island-of-inversion region is determined by the double-folding model with the Melbourne $g$-matrix and the density calculated by the antisymmetrized molecular dynamics (AMD). The double-folding model reproduces, with no adjustable parameter, the measured reaction cross sections for the scattering of $^{28-32}$Ne from $^{12}$C at 240MeV/nucleon. The quadrupole deformation thus determined is around 0.4 in the island-of-inversion region and $^{31}$Ne is a halo nuclei with large deformation. We propose the Woods-Saxon model with a suitably chosen parameterizat"},"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":"1201.2497","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2012-01-12T08:16:59Z","cross_cats_sorted":[],"title_canon_sha256":"8650197cd610b7cca8d71e248e2f64c2a50fd44596c152e0d5ce7656db206138","abstract_canon_sha256":"cd9b7ce314cec023d1da07a39d7454e732bf9ac8451f7373119f4132f895ddfb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:52.318363Z","signature_b64":"zpe3xIgX14Cihj5xpeliJcOCLCWDHZnU7cEqspWmBVsSCEqU5SlJ99/pdGvT7QDmYV1SyduWEqptjRZ/3Kb4Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0d482361714d2d539001c792e52e5f7e63d31f3e4324d4f9a58170384d73c263","last_reissued_at":"2026-05-18T01:58:52.317522Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:52.317522Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deformation of Ne isotopes in the island-of-inversion region","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Kazuyuki Ogata, Kosho Minomo, Masaaki Kimura, Masanobu Yahiro, Shingo Tagami, Takenori Sumi, Takuma Matsumoto, Yoshifumi R. Shimizu","submitted_at":"2012-01-12T08:16:59Z","abstract_excerpt":"The deformation of Ne isotopes in the island-of-inversion region is determined by the double-folding model with the Melbourne $g$-matrix and the density calculated by the antisymmetrized molecular dynamics (AMD). The double-folding model reproduces, with no adjustable parameter, the measured reaction cross sections for the scattering of $^{28-32}$Ne from $^{12}$C at 240MeV/nucleon. The quadrupole deformation thus determined is around 0.4 in the island-of-inversion region and $^{31}$Ne is a halo nuclei with large deformation. We propose the Woods-Saxon model with a suitably chosen parameterizat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1201.2497","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":"1201.2497","created_at":"2026-05-18T01:58:52.317662+00:00"},{"alias_kind":"arxiv_version","alias_value":"1201.2497v1","created_at":"2026-05-18T01:58:52.317662+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1201.2497","created_at":"2026-05-18T01:58:52.317662+00:00"},{"alias_kind":"pith_short_12","alias_value":"BVECGYLRJUWV","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_16","alias_value":"BVECGYLRJUWVHEAB","created_at":"2026-05-18T12:27:01.376967+00:00"},{"alias_kind":"pith_short_8","alias_value":"BVECGYLR","created_at":"2026-05-18T12:27:01.376967+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/BVECGYLRJUWVHEABY6JOKLS7PZ","json":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ.json","graph_json":"https://pith.science/api/pith-number/BVECGYLRJUWVHEABY6JOKLS7PZ/graph.json","events_json":"https://pith.science/api/pith-number/BVECGYLRJUWVHEABY6JOKLS7PZ/events.json","paper":"https://pith.science/paper/BVECGYLR"},"agent_actions":{"view_html":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ","download_json":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ.json","view_paper":"https://pith.science/paper/BVECGYLR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1201.2497&json=true","fetch_graph":"https://pith.science/api/pith-number/BVECGYLRJUWVHEABY6JOKLS7PZ/graph.json","fetch_events":"https://pith.science/api/pith-number/BVECGYLRJUWVHEABY6JOKLS7PZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ/action/storage_attestation","attest_author":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ/action/author_attestation","sign_citation":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ/action/citation_signature","submit_replication":"https://pith.science/pith/BVECGYLRJUWVHEABY6JOKLS7PZ/action/replication_record"}},"created_at":"2026-05-18T01:58:52.317662+00:00","updated_at":"2026-05-18T01:58:52.317662+00:00"}