{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:T2CSIJSYJQ6WCJ7OV5YPZXUYAB","short_pith_number":"pith:T2CSIJSY","schema_version":"1.0","canonical_sha256":"9e852426584c3d6127eeaf70fcde98005f0033d305166666c9a017e0df221527","source":{"kind":"arxiv","id":"1412.1997","version":2},"attestation_state":"computed","paper":{"title":"Monopole giant resonance in $^{100-132}$Sn, $^{144}$Sm and $^{208}$Pb","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Repko, D. Bozhik, J. Kvasil, P.-G. Reinhard, V.O. Nesterenko, W. Kleinig","submitted_at":"2014-12-05T13:57:55Z","abstract_excerpt":"The isoscalar giant monopole resonance (GMR) in spherical nuclei $^{100-132}$Sn, $^{144}$Sm, and $^{208}$Pb is investigated within the Skyrme random-phase-approximation (RPA) for a variety of Skyrme forces and different pairing options. The calculated GMR strength functions are directly compared to the available experimental distributions. It is shown that, in accordance to results of other groups, description of GMR in Sn and heavier Sm/Pb nuclei needs different values of the nuclear incompressibilty, $K \\approx$ 200 or 230 MeV, respectively. Thus none from the used Skyrme forces is able to d"},"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":"1412.1997","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2014-12-05T13:57:55Z","cross_cats_sorted":[],"title_canon_sha256":"0d2f88a48fc1937da9dcbb6064d95029ec57e32250abbf80ac874a00dbd4023f","abstract_canon_sha256":"d2c4d0c88d8741f1a89aea81de10284ce149e2060cee563b4e60735de175c44c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:08.687937Z","signature_b64":"K7f2t/18OUo5+CtQxke29PJ0XTxkJ+e3PcjXloJ2DbpLAg1HQMhFMerGt0i0StThX1c09/uvuXVrJ3d1MmdnBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e852426584c3d6127eeaf70fcde98005f0033d305166666c9a017e0df221527","last_reissued_at":"2026-05-18T01:21:08.687380Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:08.687380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Monopole giant resonance in $^{100-132}$Sn, $^{144}$Sm and $^{208}$Pb","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"A. Repko, D. Bozhik, J. Kvasil, P.-G. Reinhard, V.O. Nesterenko, W. Kleinig","submitted_at":"2014-12-05T13:57:55Z","abstract_excerpt":"The isoscalar giant monopole resonance (GMR) in spherical nuclei $^{100-132}$Sn, $^{144}$Sm, and $^{208}$Pb is investigated within the Skyrme random-phase-approximation (RPA) for a variety of Skyrme forces and different pairing options. The calculated GMR strength functions are directly compared to the available experimental distributions. It is shown that, in accordance to results of other groups, description of GMR in Sn and heavier Sm/Pb nuclei needs different values of the nuclear incompressibilty, $K \\approx$ 200 or 230 MeV, respectively. Thus none from the used Skyrme forces is able to d"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.1997","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":"1412.1997","created_at":"2026-05-18T01:21:08.687496+00:00"},{"alias_kind":"arxiv_version","alias_value":"1412.1997v2","created_at":"2026-05-18T01:21:08.687496+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.1997","created_at":"2026-05-18T01:21:08.687496+00:00"},{"alias_kind":"pith_short_12","alias_value":"T2CSIJSYJQ6W","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_16","alias_value":"T2CSIJSYJQ6WCJ7O","created_at":"2026-05-18T12:28:49.207871+00:00"},{"alias_kind":"pith_short_8","alias_value":"T2CSIJSY","created_at":"2026-05-18T12:28:49.207871+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/T2CSIJSYJQ6WCJ7OV5YPZXUYAB","json":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB.json","graph_json":"https://pith.science/api/pith-number/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/graph.json","events_json":"https://pith.science/api/pith-number/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/events.json","paper":"https://pith.science/paper/T2CSIJSY"},"agent_actions":{"view_html":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB","download_json":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB.json","view_paper":"https://pith.science/paper/T2CSIJSY","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1412.1997&json=true","fetch_graph":"https://pith.science/api/pith-number/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/graph.json","fetch_events":"https://pith.science/api/pith-number/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/action/storage_attestation","attest_author":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/action/author_attestation","sign_citation":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/action/citation_signature","submit_replication":"https://pith.science/pith/T2CSIJSYJQ6WCJ7OV5YPZXUYAB/action/replication_record"}},"created_at":"2026-05-18T01:21:08.687496+00:00","updated_at":"2026-05-18T01:21:08.687496+00:00"}