{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:ZFV6POX6JM4GJBBIHWIJ5Y3J7E","short_pith_number":"pith:ZFV6POX6","schema_version":"1.0","canonical_sha256":"c96be7bafe4b386484283d909ee369f905ee0cdc7ce9fcfde283f9322ce38134","source":{"kind":"arxiv","id":"1301.1461","version":2},"attestation_state":"computed","paper":{"title":"Evolution of Surface Deformations of Weakly-Bound Nuclei in the Continuum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"F. R. Xu, J. C. Pei, Y. N. Zhang","submitted_at":"2013-01-08T09:47:07Z","abstract_excerpt":"We study weakly-bound deformed nuclei based on the coordinate-space Skyrme Hartree-Fock-Bogoliubov approach, in which a large box is employed for treating the continuum and surface diffuseness. Approaching the limit of core-halo deformation decoupling, calculations found an exotic \"egg\"-like structure consisting of a spherical core plus a prolate halo in $^{38}$Ne, in which the resonant continuum plays an essential role. Generally the halo probability and the decoupling effect in heavy nuclei are reduced compared to light nuclei, due to denser level densities around Fermi surfaces. However, 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":"1301.1461","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2013-01-08T09:47:07Z","cross_cats_sorted":[],"title_canon_sha256":"0459d348395028aab6e59052a4a43bb4d729d9c5a78d8dac4eaf55bb27b3b246","abstract_canon_sha256":"47e5f527c8c3f690babe2d274f439b7f167e48c56430564df3a17de8333305cd"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:52:15.258438Z","signature_b64":"A65SZK6vPB7KNhsz/24oLxb8cwCOdO+KquyzU6/78tnx7ADsbmRhI0cn3B14hMA8UvjTnM4cb4NHcezaXa49DQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c96be7bafe4b386484283d909ee369f905ee0cdc7ce9fcfde283f9322ce38134","last_reissued_at":"2026-05-18T01:52:15.257733Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:52:15.257733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evolution of Surface Deformations of Weakly-Bound Nuclei in the Continuum","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"F. R. Xu, J. C. Pei, Y. N. Zhang","submitted_at":"2013-01-08T09:47:07Z","abstract_excerpt":"We study weakly-bound deformed nuclei based on the coordinate-space Skyrme Hartree-Fock-Bogoliubov approach, in which a large box is employed for treating the continuum and surface diffuseness. Approaching the limit of core-halo deformation decoupling, calculations found an exotic \"egg\"-like structure consisting of a spherical core plus a prolate halo in $^{38}$Ne, in which the resonant continuum plays an essential role. Generally the halo probability and the decoupling effect in heavy nuclei are reduced compared to light nuclei, due to denser level densities around Fermi surfaces. However, de"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1301.1461","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":"1301.1461","created_at":"2026-05-18T01:52:15.257848+00:00"},{"alias_kind":"arxiv_version","alias_value":"1301.1461v2","created_at":"2026-05-18T01:52:15.257848+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1301.1461","created_at":"2026-05-18T01:52:15.257848+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZFV6POX6JM4G","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZFV6POX6JM4GJBBI","created_at":"2026-05-18T12:28:09.283467+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZFV6POX6","created_at":"2026-05-18T12:28:09.283467+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/ZFV6POX6JM4GJBBIHWIJ5Y3J7E","json":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E.json","graph_json":"https://pith.science/api/pith-number/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/graph.json","events_json":"https://pith.science/api/pith-number/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/events.json","paper":"https://pith.science/paper/ZFV6POX6"},"agent_actions":{"view_html":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E","download_json":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E.json","view_paper":"https://pith.science/paper/ZFV6POX6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1301.1461&json=true","fetch_graph":"https://pith.science/api/pith-number/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/graph.json","fetch_events":"https://pith.science/api/pith-number/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/action/storage_attestation","attest_author":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/action/author_attestation","sign_citation":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/action/citation_signature","submit_replication":"https://pith.science/pith/ZFV6POX6JM4GJBBIHWIJ5Y3J7E/action/replication_record"}},"created_at":"2026-05-18T01:52:15.257848+00:00","updated_at":"2026-05-18T01:52:15.257848+00:00"}