{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2007:SBATBLJEZQ5VP7AKB2PVT7ML2W","short_pith_number":"pith:SBATBLJE","schema_version":"1.0","canonical_sha256":"904130ad24cc3b57fc0a0e9f59fd8bd590026e6318790e308f0bcfa6b26abfd2","source":{"kind":"arxiv","id":"0711.1275","version":2},"attestation_state":"computed","paper":{"title":"Halo phenomenon in finite many-fermion systems. Atom-positron complexes and large-scale study of atomic nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"K. Bennaceur (IPN Lyon), NSCL), T. Duguet (CEA), V. Rotival (CEA","submitted_at":"2007-11-08T16:38:32Z","abstract_excerpt":"The analysis method proposed in Ref. \\cite{rotival07a} is applied to characterize halo properties in finite many-fermion systems. First, the versatility of the method is highlighted by applying it to light and medium-mass nuclei as well as to atom-positron and ion-positronium complexes. Second, the dependence of nuclear halo properties on the characteristics of the energy density functional used in self-consistent Hartree-Fock-Bogoliubov calculations is studied. It is found that (a) the low-density behavior of the pairing functional and the regularization/renormalization scheme must be chosen "},"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":"0711.1275","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2007-11-08T16:38:32Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"8ef94aaa7137bbabe84e490b57173d22ff2670e5dd05e53b58bdb0d17e23f9a9","abstract_canon_sha256":"66724f12cfdb3cf59954a69fb883e92283aef5290e181cc22b233e0270329fc9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:24:18.943176Z","signature_b64":"m+PzhEDLyJnlhh3x30eBE2fJHB67PNXWwX8r6Gi5q6e7loVz3S7OzdOGu5tiXeSKLdtb4f/UvhnoXDf0OVv2Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"904130ad24cc3b57fc0a0e9f59fd8bd590026e6318790e308f0bcfa6b26abfd2","last_reissued_at":"2026-05-18T03:24:18.942609Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:24:18.942609Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Halo phenomenon in finite many-fermion systems. Atom-positron complexes and large-scale study of atomic nuclei","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"K. Bennaceur (IPN Lyon), NSCL), T. Duguet (CEA), V. Rotival (CEA","submitted_at":"2007-11-08T16:38:32Z","abstract_excerpt":"The analysis method proposed in Ref. \\cite{rotival07a} is applied to characterize halo properties in finite many-fermion systems. First, the versatility of the method is highlighted by applying it to light and medium-mass nuclei as well as to atom-positron and ion-positronium complexes. Second, the dependence of nuclear halo properties on the characteristics of the energy density functional used in self-consistent Hartree-Fock-Bogoliubov calculations is studied. It is found that (a) the low-density behavior of the pairing functional and the regularization/renormalization scheme must be chosen "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0711.1275","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":"0711.1275","created_at":"2026-05-18T03:24:18.942708+00:00"},{"alias_kind":"arxiv_version","alias_value":"0711.1275v2","created_at":"2026-05-18T03:24:18.942708+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0711.1275","created_at":"2026-05-18T03:24:18.942708+00:00"},{"alias_kind":"pith_short_12","alias_value":"SBATBLJEZQ5V","created_at":"2026-05-18T12:25:56.245647+00:00"},{"alias_kind":"pith_short_16","alias_value":"SBATBLJEZQ5VP7AK","created_at":"2026-05-18T12:25:56.245647+00:00"},{"alias_kind":"pith_short_8","alias_value":"SBATBLJE","created_at":"2026-05-18T12:25:56.245647+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/SBATBLJEZQ5VP7AKB2PVT7ML2W","json":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W.json","graph_json":"https://pith.science/api/pith-number/SBATBLJEZQ5VP7AKB2PVT7ML2W/graph.json","events_json":"https://pith.science/api/pith-number/SBATBLJEZQ5VP7AKB2PVT7ML2W/events.json","paper":"https://pith.science/paper/SBATBLJE"},"agent_actions":{"view_html":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W","download_json":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W.json","view_paper":"https://pith.science/paper/SBATBLJE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0711.1275&json=true","fetch_graph":"https://pith.science/api/pith-number/SBATBLJEZQ5VP7AKB2PVT7ML2W/graph.json","fetch_events":"https://pith.science/api/pith-number/SBATBLJEZQ5VP7AKB2PVT7ML2W/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W/action/storage_attestation","attest_author":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W/action/author_attestation","sign_citation":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W/action/citation_signature","submit_replication":"https://pith.science/pith/SBATBLJEZQ5VP7AKB2PVT7ML2W/action/replication_record"}},"created_at":"2026-05-18T03:24:18.942708+00:00","updated_at":"2026-05-18T03:24:18.942708+00:00"}