{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:XRBKBGFYWLVL4V3DM3XEYP7AEK","short_pith_number":"pith:XRBKBGFY","schema_version":"1.0","canonical_sha256":"bc42a098b8b2eabe576366ee4c3fe022a9c29909b1ba63dd0b42112ff4a504e8","source":{"kind":"arxiv","id":"2607.21730","version":1},"attestation_state":"computed","paper":{"title":"Deformation, halo, and bubble structure: A paradigm shift of exotic phenomena in light to medium mass nuclei","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"G. Singh, Jagjit Singh, M. Kimura, R. Barman, R. Chatterjee, Shubhchintak, W. Horiuchi","submitted_at":"2026-07-23T18:27:53Z","abstract_excerpt":"The emergence of exotic nuclear structures, such as deformation, one- and two-neutron halos, and bubble configurations, marks a paradigm shift in our understanding of light- to medium-mass nuclei far from stability, particularly near and within the island of inversion extending across $N=20-28$. In this review, we integrate microscopic structure calculations using the antisymmetrized molecular dynamics method with reaction theories such as the Glauber model for high-energy collisions, and highlight the use of the fully quantum mechanical finite-range distorted wave Born approximation for calcu"},"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":"2607.21730","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","primary_cat":"nucl-th","submitted_at":"2026-07-23T18:27:53Z","cross_cats_sorted":[],"title_canon_sha256":"cacab6089ead26d17d618975c75a9122d7c473109e29cee6f3bb860db9d6e510","abstract_canon_sha256":"6f62ca5616f049562913fc06d7dcfec6e69b5e66d877b9895198aa53b1d792c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-27T00:20:17.863939Z","signature_b64":"jJA5eVEuXTU6a3EY2PxebFEUNfK8SzHz9wL6tMQLSGrInkGH7oQ2KEIsmwnAdMPQhu8LjSPfgTYyVxEpe6usDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"bc42a098b8b2eabe576366ee4c3fe022a9c29909b1ba63dd0b42112ff4a504e8","last_reissued_at":"2026-07-27T00:20:17.863096Z","signature_status":"signed_v1","first_computed_at":"2026-07-27T00:20:17.863096Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Deformation, halo, and bubble structure: A paradigm shift of exotic phenomena in light to medium mass nuclei","license":"http://creativecommons.org/licenses/by-nc-nd/4.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"G. Singh, Jagjit Singh, M. Kimura, R. Barman, R. Chatterjee, Shubhchintak, W. Horiuchi","submitted_at":"2026-07-23T18:27:53Z","abstract_excerpt":"The emergence of exotic nuclear structures, such as deformation, one- and two-neutron halos, and bubble configurations, marks a paradigm shift in our understanding of light- to medium-mass nuclei far from stability, particularly near and within the island of inversion extending across $N=20-28$. In this review, we integrate microscopic structure calculations using the antisymmetrized molecular dynamics method with reaction theories such as the Glauber model for high-energy collisions, and highlight the use of the fully quantum mechanical finite-range distorted wave Born approximation for calcu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2607.21730","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2607.21730/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":"2607.21730","created_at":"2026-07-27T00:20:17.863541+00:00"},{"alias_kind":"arxiv_version","alias_value":"2607.21730v1","created_at":"2026-07-27T00:20:17.863541+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2607.21730","created_at":"2026-07-27T00:20:17.863541+00:00"},{"alias_kind":"pith_short_12","alias_value":"XRBKBGFYWLVL","created_at":"2026-07-27T00:20:17.863541+00:00"},{"alias_kind":"pith_short_16","alias_value":"XRBKBGFYWLVL4V3D","created_at":"2026-07-27T00:20:17.863541+00:00"},{"alias_kind":"pith_short_8","alias_value":"XRBKBGFY","created_at":"2026-07-27T00:20:17.863541+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/XRBKBGFYWLVL4V3DM3XEYP7AEK","json":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK.json","graph_json":"https://pith.science/api/pith-number/XRBKBGFYWLVL4V3DM3XEYP7AEK/graph.json","events_json":"https://pith.science/api/pith-number/XRBKBGFYWLVL4V3DM3XEYP7AEK/events.json","paper":"https://pith.science/paper/XRBKBGFY"},"agent_actions":{"view_html":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK","download_json":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK.json","view_paper":"https://pith.science/paper/XRBKBGFY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2607.21730&json=true","fetch_graph":"https://pith.science/api/pith-number/XRBKBGFYWLVL4V3DM3XEYP7AEK/graph.json","fetch_events":"https://pith.science/api/pith-number/XRBKBGFYWLVL4V3DM3XEYP7AEK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK/action/storage_attestation","attest_author":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK/action/author_attestation","sign_citation":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK/action/citation_signature","submit_replication":"https://pith.science/pith/XRBKBGFYWLVL4V3DM3XEYP7AEK/action/replication_record"}},"created_at":"2026-07-27T00:20:17.863541+00:00","updated_at":"2026-07-27T00:20:17.863541+00:00"}