{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:JGNJOJSFY3NWTGCXICLVNXAVOG","short_pith_number":"pith:JGNJOJSF","schema_version":"1.0","canonical_sha256":"499a972645c6db699857409756dc157182a46bb7eff305f9dbbee692b04377ff","source":{"kind":"arxiv","id":"nucl-th/0606054","version":1},"attestation_state":"computed","paper":{"title":"Relativistic QRPA description of isoscalar compression modes in open-shell nuclei in the A$\\approx$60 mass region","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"D. Vretenar, N. Paar, P. Ring, T. Niksic","submitted_at":"2006-06-27T09:23:10Z","abstract_excerpt":"Very recent inelastic $\\alpha$-scattering data on the isoscalar monopole and dipole strength distributions in $^{56}$Fe, $^{58}$Ni, and $^{60}$Ni are analyzed in the relativistic quasiparticle random-phase approximation (RQRPA) with the DD-ME2 effective nuclear interaction (nuclear matter compression modulus K$_{nm}= 251$ MeV). In all three nuclei the calculation nicely reproduces the observed asymmetric shapes of the monopole strength, and the bimodal structure of the dipole strength distributions. The calculated centroid and mean energies are in very good qualitative agreement with the exper"},"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/0606054","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-06-27T09:23:10Z","cross_cats_sorted":[],"title_canon_sha256":"9ca13cd4744b716a08a59f82a2574ce6198115b710ffb4cc366017d009648052","abstract_canon_sha256":"fa6e77bcb91303386b40c64db5e56fae65027be91831230bc27662d0a3018c21"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:02:22.181893Z","signature_b64":"5AKDZNUZ66snCE7hzTVQIn+4BFZlwfBKA1pO3VbnDmkYm1OWeuw5tjAoFhrNudnMSTKXx21lvpiIJMf0kPhkDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"499a972645c6db699857409756dc157182a46bb7eff305f9dbbee692b04377ff","last_reissued_at":"2026-07-04T17:02:22.181516Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:02:22.181516Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Relativistic QRPA description of isoscalar compression modes in open-shell nuclei in the A$\\approx$60 mass region","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"D. Vretenar, N. Paar, P. Ring, T. Niksic","submitted_at":"2006-06-27T09:23:10Z","abstract_excerpt":"Very recent inelastic $\\alpha$-scattering data on the isoscalar monopole and dipole strength distributions in $^{56}$Fe, $^{58}$Ni, and $^{60}$Ni are analyzed in the relativistic quasiparticle random-phase approximation (RQRPA) with the DD-ME2 effective nuclear interaction (nuclear matter compression modulus K$_{nm}= 251$ MeV). In all three nuclei the calculation nicely reproduces the observed asymmetric shapes of the monopole strength, and the bimodal structure of the dipole strength distributions. The calculated centroid and mean energies are in very good qualitative agreement with the exper"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0606054","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/0606054/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/0606054","created_at":"2026-07-04T17:02:22.181575+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0606054v1","created_at":"2026-07-04T17:02:22.181575+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0606054","created_at":"2026-07-04T17:02:22.181575+00:00"},{"alias_kind":"pith_short_12","alias_value":"JGNJOJSFY3NW","created_at":"2026-07-04T17:02:22.181575+00:00"},{"alias_kind":"pith_short_16","alias_value":"JGNJOJSFY3NWTGCX","created_at":"2026-07-04T17:02:22.181575+00:00"},{"alias_kind":"pith_short_8","alias_value":"JGNJOJSF","created_at":"2026-07-04T17:02:22.181575+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/JGNJOJSFY3NWTGCXICLVNXAVOG","json":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG.json","graph_json":"https://pith.science/api/pith-number/JGNJOJSFY3NWTGCXICLVNXAVOG/graph.json","events_json":"https://pith.science/api/pith-number/JGNJOJSFY3NWTGCXICLVNXAVOG/events.json","paper":"https://pith.science/paper/JGNJOJSF"},"agent_actions":{"view_html":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG","download_json":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG.json","view_paper":"https://pith.science/paper/JGNJOJSF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0606054&json=true","fetch_graph":"https://pith.science/api/pith-number/JGNJOJSFY3NWTGCXICLVNXAVOG/graph.json","fetch_events":"https://pith.science/api/pith-number/JGNJOJSFY3NWTGCXICLVNXAVOG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG/action/storage_attestation","attest_author":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG/action/author_attestation","sign_citation":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG/action/citation_signature","submit_replication":"https://pith.science/pith/JGNJOJSFY3NWTGCXICLVNXAVOG/action/replication_record"}},"created_at":"2026-07-04T17:02:22.181575+00:00","updated_at":"2026-07-04T17:02:22.181575+00:00"}