{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:5YHDYE6TX45HMIPJIICOOMCFGQ","short_pith_number":"pith:5YHDYE6T","schema_version":"1.0","canonical_sha256":"ee0e3c13d3bf3a7621e94204e730453438e22ddc75cce94054a8b6dae884d9d4","source":{"kind":"arxiv","id":"nucl-th/0511041","version":1},"attestation_state":"computed","paper":{"title":"Self-Consistent Description of Collective Excitations in the Unitary Correlation Operator Method","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Hergert, N. Paar, P. Papakonstantinou, R. Roth","submitted_at":"2005-11-16T15:06:14Z","abstract_excerpt":"The fully self-consistent Random Phase Approximation (RPA) is constructed within the Unitary Correlation Operator Method (UCOM), which describes the dominant interaction-induced short-range central and tensor correlations by a unitary transformation. Based on the correlated Argonne V18 interaction, the RPA is employed in studies of multipole response in closed-shell nuclei across the nuclide chart. The UCOM-RPA results in a collective character of giant resonances, and it describes rather well the properties of isoscalar giant monopole resonances. However, the excitation energies of isovector "},"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/0511041","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2005-11-16T15:06:14Z","cross_cats_sorted":[],"title_canon_sha256":"1645136a1c44db0f07dfb8442c1ef921e99ce9e951908de098d9788016cf070a","abstract_canon_sha256":"e68ab0a45585c3c3917c4d6c03b068443c8f35204d96296d34f51db258f7bddb"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:57:01.322093Z","signature_b64":"KYZWX1tZotsowJAG4TMZSjoIeil6TSKsyIRRpdvUiL+Odevx4JLHSTLJuNLcSoCzDot4RQsVwxHN0+ayTuZKBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ee0e3c13d3bf3a7621e94204e730453438e22ddc75cce94054a8b6dae884d9d4","last_reissued_at":"2026-07-04T16:57:01.321738Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:57:01.321738Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Self-Consistent Description of Collective Excitations in the Unitary Correlation Operator Method","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"H. Hergert, N. Paar, P. Papakonstantinou, R. Roth","submitted_at":"2005-11-16T15:06:14Z","abstract_excerpt":"The fully self-consistent Random Phase Approximation (RPA) is constructed within the Unitary Correlation Operator Method (UCOM), which describes the dominant interaction-induced short-range central and tensor correlations by a unitary transformation. Based on the correlated Argonne V18 interaction, the RPA is employed in studies of multipole response in closed-shell nuclei across the nuclide chart. The UCOM-RPA results in a collective character of giant resonances, and it describes rather well the properties of isoscalar giant monopole resonances. However, the excitation energies of isovector "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0511041","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/nucl-th/0511041/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":"nucl-th/0511041","created_at":"2026-07-04T16:57:01.321802+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0511041v1","created_at":"2026-07-04T16:57:01.321802+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0511041","created_at":"2026-07-04T16:57:01.321802+00:00"},{"alias_kind":"pith_short_12","alias_value":"5YHDYE6TX45H","created_at":"2026-07-04T16:57:01.321802+00:00"},{"alias_kind":"pith_short_16","alias_value":"5YHDYE6TX45HMIPJ","created_at":"2026-07-04T16:57:01.321802+00:00"},{"alias_kind":"pith_short_8","alias_value":"5YHDYE6T","created_at":"2026-07-04T16:57:01.321802+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/5YHDYE6TX45HMIPJIICOOMCFGQ","json":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ.json","graph_json":"https://pith.science/api/pith-number/5YHDYE6TX45HMIPJIICOOMCFGQ/graph.json","events_json":"https://pith.science/api/pith-number/5YHDYE6TX45HMIPJIICOOMCFGQ/events.json","paper":"https://pith.science/paper/5YHDYE6T"},"agent_actions":{"view_html":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ","download_json":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ.json","view_paper":"https://pith.science/paper/5YHDYE6T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0511041&json=true","fetch_graph":"https://pith.science/api/pith-number/5YHDYE6TX45HMIPJIICOOMCFGQ/graph.json","fetch_events":"https://pith.science/api/pith-number/5YHDYE6TX45HMIPJIICOOMCFGQ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ/action/storage_attestation","attest_author":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ/action/author_attestation","sign_citation":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ/action/citation_signature","submit_replication":"https://pith.science/pith/5YHDYE6TX45HMIPJIICOOMCFGQ/action/replication_record"}},"created_at":"2026-07-04T16:57:01.321802+00:00","updated_at":"2026-07-04T16:57:01.321802+00:00"}