{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:MUN4ZJGQKBI562QWSHOVVGV2GC","short_pith_number":"pith:MUN4ZJGQ","schema_version":"1.0","canonical_sha256":"651bcca4d05051df6a1691dd5a9aba3085d9bd485bf4772d50054e8aae91169e","source":{"kind":"arxiv","id":"nucl-th/0602035","version":2},"attestation_state":"computed","paper":{"title":"Gamow shell model and realistic nucleon-nucleon interactions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"G. Hagen, M. Hjorth-Jensen, N. Michel","submitted_at":"2006-02-10T21:44:59Z","abstract_excerpt":"We present a new and efficient method to obtain a Gamow shell-model basis and matrix elements generated by realistic nucleon-nucleon interactions. We derive a self-consistent Hartree-Fock potential from the renormalized N3LO interaction model. The corresponding Gamow one-body eigenstates are generated in a plane wave basis in order to build a Gamow shell-model set of basis states for the closed shell nuclei 4He and 16O. We address also the problem of representing a realistic nucleon-nucleon interaction in a two-particle Berggren basis in the laboratory frame. To achieve this, an expansion of m"},"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":"nucl-th/0602035","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-02-10T21:44:59Z","cross_cats_sorted":[],"title_canon_sha256":"d50077d7467d49e7a4965f723830896b89185de34ad61e7233b002822090951c","abstract_canon_sha256":"99adcf62b42eafab12e79f4ed57490c56431c5a75ab7b88a959d537b58d4bd26"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:17:54.313357Z","signature_b64":"65CMJHJ9rvaCkGae5/4PB5vDsuY+rLAM/vIv0B5mG4JbIwqTkyzy+nkuot02a73JNafzkNBIiRwMM2/ld1GvDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"651bcca4d05051df6a1691dd5a9aba3085d9bd485bf4772d50054e8aae91169e","last_reissued_at":"2026-05-18T04:17:54.312791Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:17:54.312791Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gamow shell model and realistic nucleon-nucleon interactions","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"G. Hagen, M. Hjorth-Jensen, N. Michel","submitted_at":"2006-02-10T21:44:59Z","abstract_excerpt":"We present a new and efficient method to obtain a Gamow shell-model basis and matrix elements generated by realistic nucleon-nucleon interactions. We derive a self-consistent Hartree-Fock potential from the renormalized N3LO interaction model. The corresponding Gamow one-body eigenstates are generated in a plane wave basis in order to build a Gamow shell-model set of basis states for the closed shell nuclei 4He and 16O. We address also the problem of representing a realistic nucleon-nucleon interaction in a two-particle Berggren basis in the laboratory frame. To achieve this, an expansion of m"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0602035","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":"nucl-th/0602035","created_at":"2026-05-18T04:17:54.312878+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0602035v2","created_at":"2026-05-18T04:17:54.312878+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0602035","created_at":"2026-05-18T04:17:54.312878+00:00"},{"alias_kind":"pith_short_12","alias_value":"MUN4ZJGQKBI5","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_16","alias_value":"MUN4ZJGQKBI562QW","created_at":"2026-05-18T12:25:54.717736+00:00"},{"alias_kind":"pith_short_8","alias_value":"MUN4ZJGQ","created_at":"2026-05-18T12:25:54.717736+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/MUN4ZJGQKBI562QWSHOVVGV2GC","json":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC.json","graph_json":"https://pith.science/api/pith-number/MUN4ZJGQKBI562QWSHOVVGV2GC/graph.json","events_json":"https://pith.science/api/pith-number/MUN4ZJGQKBI562QWSHOVVGV2GC/events.json","paper":"https://pith.science/paper/MUN4ZJGQ"},"agent_actions":{"view_html":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC","download_json":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC.json","view_paper":"https://pith.science/paper/MUN4ZJGQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0602035&json=true","fetch_graph":"https://pith.science/api/pith-number/MUN4ZJGQKBI562QWSHOVVGV2GC/graph.json","fetch_events":"https://pith.science/api/pith-number/MUN4ZJGQKBI562QWSHOVVGV2GC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC/action/storage_attestation","attest_author":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC/action/author_attestation","sign_citation":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC/action/citation_signature","submit_replication":"https://pith.science/pith/MUN4ZJGQKBI562QWSHOVVGV2GC/action/replication_record"}},"created_at":"2026-05-18T04:17:54.312878+00:00","updated_at":"2026-05-18T04:17:54.312878+00:00"}