{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:KNYRQAHYBXDANCYVVD6CITQLQQ","short_pith_number":"pith:KNYRQAHY","schema_version":"1.0","canonical_sha256":"53711800f80dc6068b15a8fc244e0b84023b5004eb0d8cbdc12674d29c23faac","source":{"kind":"arxiv","id":"1106.2022","version":2},"attestation_state":"computed","paper":{"title":"On a translationally invariant nuclear single particle picture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"(2) Kyushu Institute of Technology, (3) Jagiellonian University Krakow), H. Kamada (2), J. Golak (3) ((1) Ruhr-Universitaet Bochum, W. Gloeckle (1)","submitted_at":"2011-06-10T11:47:59Z","abstract_excerpt":"If one assumes a translationally invariant motion of the nucleons relative to the c. m. position in single particle mean fields a correlated single particle picture of the nuclear wave function emerges. A single particle product ansatz leads for that Hamiltonian to nonlinear equations for the single particle wave functions. In contrast to a standard not translationally invariant shell model picture those single particle s-, p- etc states are coupled. The strength of the resulting coupling is an open question. The Schroedinger equation for that Hamiltonian can be solved by few- and many -body t"},"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":"1106.2022","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2011-06-10T11:47:59Z","cross_cats_sorted":[],"title_canon_sha256":"f34608592811c9f6757cf4667cbba30511d2641324583ac430137f78a78398f4","abstract_canon_sha256":"fed309523356ed719874707c8227a1cf47938fe9ba2ad9547de1d978feb398db"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:20:06.315859Z","signature_b64":"L1zSAVpoXPcYhyNm3jBCldDGczcc/0NquxebRZev/H58u0u8K6ESfugC7CbczTs+JSX4kk0PGWpi8ECygoFSCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"53711800f80dc6068b15a8fc244e0b84023b5004eb0d8cbdc12674d29c23faac","last_reissued_at":"2026-05-18T04:20:06.315453Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:20:06.315453Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On a translationally invariant nuclear single particle picture","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"(2) Kyushu Institute of Technology, (3) Jagiellonian University Krakow), H. Kamada (2), J. Golak (3) ((1) Ruhr-Universitaet Bochum, W. Gloeckle (1)","submitted_at":"2011-06-10T11:47:59Z","abstract_excerpt":"If one assumes a translationally invariant motion of the nucleons relative to the c. m. position in single particle mean fields a correlated single particle picture of the nuclear wave function emerges. A single particle product ansatz leads for that Hamiltonian to nonlinear equations for the single particle wave functions. In contrast to a standard not translationally invariant shell model picture those single particle s-, p- etc states are coupled. The strength of the resulting coupling is an open question. The Schroedinger equation for that Hamiltonian can be solved by few- and many -body t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1106.2022","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":"1106.2022","created_at":"2026-05-18T04:20:06.315515+00:00"},{"alias_kind":"arxiv_version","alias_value":"1106.2022v2","created_at":"2026-05-18T04:20:06.315515+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1106.2022","created_at":"2026-05-18T04:20:06.315515+00:00"},{"alias_kind":"pith_short_12","alias_value":"KNYRQAHYBXDA","created_at":"2026-05-18T12:26:32.869790+00:00"},{"alias_kind":"pith_short_16","alias_value":"KNYRQAHYBXDANCYV","created_at":"2026-05-18T12:26:32.869790+00:00"},{"alias_kind":"pith_short_8","alias_value":"KNYRQAHY","created_at":"2026-05-18T12:26:32.869790+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/KNYRQAHYBXDANCYVVD6CITQLQQ","json":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ.json","graph_json":"https://pith.science/api/pith-number/KNYRQAHYBXDANCYVVD6CITQLQQ/graph.json","events_json":"https://pith.science/api/pith-number/KNYRQAHYBXDANCYVVD6CITQLQQ/events.json","paper":"https://pith.science/paper/KNYRQAHY"},"agent_actions":{"view_html":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ","download_json":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ.json","view_paper":"https://pith.science/paper/KNYRQAHY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1106.2022&json=true","fetch_graph":"https://pith.science/api/pith-number/KNYRQAHYBXDANCYVVD6CITQLQQ/graph.json","fetch_events":"https://pith.science/api/pith-number/KNYRQAHYBXDANCYVVD6CITQLQQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ/action/storage_attestation","attest_author":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ/action/author_attestation","sign_citation":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ/action/citation_signature","submit_replication":"https://pith.science/pith/KNYRQAHYBXDANCYVVD6CITQLQQ/action/replication_record"}},"created_at":"2026-05-18T04:20:06.315515+00:00","updated_at":"2026-05-18T04:20:06.315515+00:00"}