{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:4E2CCUDGH4YQVIVKI6MQTLKFXB","short_pith_number":"pith:4E2CCUDG","schema_version":"1.0","canonical_sha256":"e1342150663f310aa2aa479909ad45b87ba6f77525604882dce1c2f0e2f58e25","source":{"kind":"arxiv","id":"1305.3360","version":1},"attestation_state":"computed","paper":{"title":"Giant dipole resonance width as a probe for nuclear deformation at finite excitation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. De, Balaram Dey, Debasish Mondal, Deepak Pandit, S. Mukhopadhyay, S. R. Banerjee, Srijit Bhattacharya, Surajit Pal","submitted_at":"2013-05-15T05:48:56Z","abstract_excerpt":"The systematic study of the correlation between the experimental giant dipole resonance (GDR) width and the average deformation <\\beta> of the nucleus at finite excitation is presented for the mass region A ~ 59 to 208. We show that the width of the GDR (\\Gamma) and the quadrupole deformation of the nucleus do not follow a linear relation, as predicted earlier, due to the GDR induced quadrupole moment and the correlation also depends on the mass of the nuclei. The different empirical values of <\\beta> extracted from the experimental GDR width match exceptionally well with the thermal shape flu"},"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":"1305.3360","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-ex","submitted_at":"2013-05-15T05:48:56Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"bad170433ca96065a03c307b88a4df3be36954989f5a3b292db9dacf92650668","abstract_canon_sha256":"27af883dfaa344e9512a694708de6fc6a89f742cdf3379fa06f1ddbdcf0fa4b9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:25:36.038265Z","signature_b64":"iySFSy331Qc7uQ3nRtZGvAimUVJ0u4xab8VwOns9HH8P/APQjo2ghMS3NDWZJ03GHsuG+/Wb8jwJjS08yiS9BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1342150663f310aa2aa479909ad45b87ba6f77525604882dce1c2f0e2f58e25","last_reissued_at":"2026-05-18T03:25:36.037791Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:25:36.037791Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Giant dipole resonance width as a probe for nuclear deformation at finite excitation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"nucl-ex","authors_text":"A. De, Balaram Dey, Debasish Mondal, Deepak Pandit, S. Mukhopadhyay, S. R. Banerjee, Srijit Bhattacharya, Surajit Pal","submitted_at":"2013-05-15T05:48:56Z","abstract_excerpt":"The systematic study of the correlation between the experimental giant dipole resonance (GDR) width and the average deformation <\\beta> of the nucleus at finite excitation is presented for the mass region A ~ 59 to 208. We show that the width of the GDR (\\Gamma) and the quadrupole deformation of the nucleus do not follow a linear relation, as predicted earlier, due to the GDR induced quadrupole moment and the correlation also depends on the mass of the nuclei. The different empirical values of <\\beta> extracted from the experimental GDR width match exceptionally well with the thermal shape flu"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1305.3360","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":""},"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":"1305.3360","created_at":"2026-05-18T03:25:36.037863+00:00"},{"alias_kind":"arxiv_version","alias_value":"1305.3360v1","created_at":"2026-05-18T03:25:36.037863+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1305.3360","created_at":"2026-05-18T03:25:36.037863+00:00"},{"alias_kind":"pith_short_12","alias_value":"4E2CCUDGH4YQ","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_16","alias_value":"4E2CCUDGH4YQVIVK","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_8","alias_value":"4E2CCUDG","created_at":"2026-05-18T12:27:32.513160+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/4E2CCUDGH4YQVIVKI6MQTLKFXB","json":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB.json","graph_json":"https://pith.science/api/pith-number/4E2CCUDGH4YQVIVKI6MQTLKFXB/graph.json","events_json":"https://pith.science/api/pith-number/4E2CCUDGH4YQVIVKI6MQTLKFXB/events.json","paper":"https://pith.science/paper/4E2CCUDG"},"agent_actions":{"view_html":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB","download_json":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB.json","view_paper":"https://pith.science/paper/4E2CCUDG","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1305.3360&json=true","fetch_graph":"https://pith.science/api/pith-number/4E2CCUDGH4YQVIVKI6MQTLKFXB/graph.json","fetch_events":"https://pith.science/api/pith-number/4E2CCUDGH4YQVIVKI6MQTLKFXB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB/action/storage_attestation","attest_author":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB/action/author_attestation","sign_citation":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB/action/citation_signature","submit_replication":"https://pith.science/pith/4E2CCUDGH4YQVIVKI6MQTLKFXB/action/replication_record"}},"created_at":"2026-05-18T03:25:36.037863+00:00","updated_at":"2026-05-18T03:25:36.037863+00:00"}