{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2020:BNYISTNP2JN77KGO7JU5BKHRF2","short_pith_number":"pith:BNYISTNP","schema_version":"1.0","canonical_sha256":"0b70894dafd25bffa8cefa69d0a8f12e86f42e536678588dd3b56477514fb76c","source":{"kind":"arxiv","id":"2012.05036","version":1},"attestation_state":"computed","paper":{"title":"Role of exact treatment of thermal pairing in radiative strength functions of $^{161-163}$Dy nuclei","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"L. Ngoc Uyen, L. Tan Phuc, L. T. Quynh Huong, N. Dinh Dang, N. Ngoc Anh, N. Ngoc Duy, N. Nhu Le, N. Quang Hung","submitted_at":"2020-12-09T13:27:16Z","abstract_excerpt":"The enhancement of radiative strength function (RSF) in the region of low $\\gamma$-rays energy ($E_{\\gamma}\\leq 12$ MeV), which is caused by the pygmy dipole resonance (PDR), is treated within the phonon damping model (PDM) plus exact thermal pairing (EP) without adding any extra PDR strength function. The numerical calculations performed for $^{161-163}$Dy show that, because of the effect of EP, the EP+PDM can describe reasonably well the total RSF data in both low- and high-energy regions of $\\gamma$-rays. Consequently, as compared to the conventional description within the phenomenological "},"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":"2012.05036","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"nucl-th","submitted_at":"2020-12-09T13:27:16Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"dbf7d51aa34db7258673a36395407c48abeb4d4f08c83970866e5b5e8f415055","abstract_canon_sha256":"f7942da95baab870131494f8a6a523ae49f37e29bd73cc8be325cebcea73a09c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:58:18.152542Z","signature_b64":"Zag85QbtwmXIVGB5Ene1CsKz4/4UzqrUotYYVGown3wlQkt/Eo3GSCnxsTZ5cmbZe1acIdJUKpz+a6T16A+6AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0b70894dafd25bffa8cefa69d0a8f12e86f42e536678588dd3b56477514fb76c","last_reissued_at":"2026-07-05T01:58:18.152049Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:58:18.152049Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Role of exact treatment of thermal pairing in radiative strength functions of $^{161-163}$Dy nuclei","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"L. Ngoc Uyen, L. Tan Phuc, L. T. Quynh Huong, N. Dinh Dang, N. Ngoc Anh, N. Ngoc Duy, N. Nhu Le, N. Quang Hung","submitted_at":"2020-12-09T13:27:16Z","abstract_excerpt":"The enhancement of radiative strength function (RSF) in the region of low $\\gamma$-rays energy ($E_{\\gamma}\\leq 12$ MeV), which is caused by the pygmy dipole resonance (PDR), is treated within the phonon damping model (PDM) plus exact thermal pairing (EP) without adding any extra PDR strength function. The numerical calculations performed for $^{161-163}$Dy show that, because of the effect of EP, the EP+PDM can describe reasonably well the total RSF data in both low- and high-energy regions of $\\gamma$-rays. Consequently, as compared to the conventional description within the phenomenological "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2012.05036","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/2012.05036/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":"2012.05036","created_at":"2026-07-05T01:58:18.152106+00:00"},{"alias_kind":"arxiv_version","alias_value":"2012.05036v1","created_at":"2026-07-05T01:58:18.152106+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2012.05036","created_at":"2026-07-05T01:58:18.152106+00:00"},{"alias_kind":"pith_short_12","alias_value":"BNYISTNP2JN7","created_at":"2026-07-05T01:58:18.152106+00:00"},{"alias_kind":"pith_short_16","alias_value":"BNYISTNP2JN77KGO","created_at":"2026-07-05T01:58:18.152106+00:00"},{"alias_kind":"pith_short_8","alias_value":"BNYISTNP","created_at":"2026-07-05T01:58:18.152106+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/BNYISTNP2JN77KGO7JU5BKHRF2","json":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2.json","graph_json":"https://pith.science/api/pith-number/BNYISTNP2JN77KGO7JU5BKHRF2/graph.json","events_json":"https://pith.science/api/pith-number/BNYISTNP2JN77KGO7JU5BKHRF2/events.json","paper":"https://pith.science/paper/BNYISTNP"},"agent_actions":{"view_html":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2","download_json":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2.json","view_paper":"https://pith.science/paper/BNYISTNP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2012.05036&json=true","fetch_graph":"https://pith.science/api/pith-number/BNYISTNP2JN77KGO7JU5BKHRF2/graph.json","fetch_events":"https://pith.science/api/pith-number/BNYISTNP2JN77KGO7JU5BKHRF2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2/action/storage_attestation","attest_author":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2/action/author_attestation","sign_citation":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2/action/citation_signature","submit_replication":"https://pith.science/pith/BNYISTNP2JN77KGO7JU5BKHRF2/action/replication_record"}},"created_at":"2026-07-05T01:58:18.152106+00:00","updated_at":"2026-07-05T01:58:18.152106+00:00"}