{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:H3QDNRH2BQTFSYATS3TSOZJ2LZ","short_pith_number":"pith:H3QDNRH2","schema_version":"1.0","canonical_sha256":"3ee036c4fa0c2659601396e727653a5e5313bbb3421454b98560eed37bb72a8e","source":{"kind":"arxiv","id":"1811.00949","version":1},"attestation_state":"computed","paper":{"title":"Anti-bubble effect of temperature \\& deformation: a systematic study for nuclei across all mass regions between A $=$ 20$-$300","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"G. Saxena, Mamta Aggarwal, M. Kumawat","submitted_at":"2018-11-02T15:59:28Z","abstract_excerpt":"Temperature dependent relativistic mean-field (RMF) plus BCS approach has been used for the first time to investigate the anti-bubble effect of the temperature and deformation in the light, medium-heavy and superheavy nuclei. Influence of temperature is studied on density distribution, charge form-factor, single particle (s.p.) energies, occupancy, deformation and the depletion fraction (DF). At T $=$ 0, the quenching effect of deformation is predominant. DF is found usually less in oblate deformation than in prolate. DF decreases with increasing prolate deformation even though the 2s-orbit is"},"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":"1811.00949","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2018-11-02T15:59:28Z","cross_cats_sorted":["nucl-ex"],"title_canon_sha256":"4b33b08e8baa19c06afb5294f3e4a47b05ffc5d0c1595513c238952c3afa2719","abstract_canon_sha256":"587a04b1198a3fb8b67a210a8d1b94ca746f60cf80643c7f2f21fcff99e25131"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:55:11.178511Z","signature_b64":"RYXt8Yh7/ypmTRVKZ0qEuFn6zdb9RnDivCuHmVGh7yZih9SttfENwdWOUd4UTv6A562qzcz78GWvuUdPUKq/BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ee036c4fa0c2659601396e727653a5e5313bbb3421454b98560eed37bb72a8e","last_reissued_at":"2026-05-17T23:55:11.178004Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:55:11.178004Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Anti-bubble effect of temperature \\& deformation: a systematic study for nuclei across all mass regions between A $=$ 20$-$300","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-ex"],"primary_cat":"nucl-th","authors_text":"G. Saxena, Mamta Aggarwal, M. Kumawat","submitted_at":"2018-11-02T15:59:28Z","abstract_excerpt":"Temperature dependent relativistic mean-field (RMF) plus BCS approach has been used for the first time to investigate the anti-bubble effect of the temperature and deformation in the light, medium-heavy and superheavy nuclei. Influence of temperature is studied on density distribution, charge form-factor, single particle (s.p.) energies, occupancy, deformation and the depletion fraction (DF). At T $=$ 0, the quenching effect of deformation is predominant. DF is found usually less in oblate deformation than in prolate. DF decreases with increasing prolate deformation even though the 2s-orbit is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.00949","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":"1811.00949","created_at":"2026-05-17T23:55:11.178076+00:00"},{"alias_kind":"arxiv_version","alias_value":"1811.00949v1","created_at":"2026-05-17T23:55:11.178076+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1811.00949","created_at":"2026-05-17T23:55:11.178076+00:00"},{"alias_kind":"pith_short_12","alias_value":"H3QDNRH2BQTF","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_16","alias_value":"H3QDNRH2BQTFSYAT","created_at":"2026-05-18T12:32:28.185984+00:00"},{"alias_kind":"pith_short_8","alias_value":"H3QDNRH2","created_at":"2026-05-18T12:32:28.185984+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/H3QDNRH2BQTFSYATS3TSOZJ2LZ","json":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ.json","graph_json":"https://pith.science/api/pith-number/H3QDNRH2BQTFSYATS3TSOZJ2LZ/graph.json","events_json":"https://pith.science/api/pith-number/H3QDNRH2BQTFSYATS3TSOZJ2LZ/events.json","paper":"https://pith.science/paper/H3QDNRH2"},"agent_actions":{"view_html":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ","download_json":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ.json","view_paper":"https://pith.science/paper/H3QDNRH2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1811.00949&json=true","fetch_graph":"https://pith.science/api/pith-number/H3QDNRH2BQTFSYATS3TSOZJ2LZ/graph.json","fetch_events":"https://pith.science/api/pith-number/H3QDNRH2BQTFSYATS3TSOZJ2LZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ/action/storage_attestation","attest_author":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ/action/author_attestation","sign_citation":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ/action/citation_signature","submit_replication":"https://pith.science/pith/H3QDNRH2BQTFSYATS3TSOZJ2LZ/action/replication_record"}},"created_at":"2026-05-17T23:55:11.178076+00:00","updated_at":"2026-05-17T23:55:11.178076+00:00"}