{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:KSBIRCT6DLOABY3DAKC6MRQJLO","short_pith_number":"pith:KSBIRCT6","schema_version":"1.0","canonical_sha256":"5482888a7e1adc00e3630285e646095b8348d19dfc3154629937b7843e032a59","source":{"kind":"arxiv","id":"1901.01852","version":1},"attestation_state":"computed","paper":{"title":"Tunneling radiation of fermions from the non-stationary Kerr black hole","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"Qun-Chao Ding, Shu-Zheng Yang, Zhong-Wen Feng","submitted_at":"2019-01-02T08:23:37Z","abstract_excerpt":"In this paper, the tunneling radiation of fermions with spin $1/2$ and $3/2$ from the non-stationary Kerr black hole are investigated. First, according to the Dirac equation for spin $1/2$ fermions and Rarita-Schwinger equation for spin $3/2$ fermions, we construct the corresponding gamma matrixes and the derive Hamilton-Jacobi equation for spin $1/2$ and $3/2$ fermions. Then, the tunneling behavior of fermions on the event horizon is studied. Finally, we obtain the thermodynamic properties of the non-stationary Kerr black hole. The result shows that the tunneling radiation rate, surface gravi"},"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":"1901.01852","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by-sa/4.0/","primary_cat":"physics.gen-ph","submitted_at":"2019-01-02T08:23:37Z","cross_cats_sorted":[],"title_canon_sha256":"9ae4dea725eb70499ef55fe720e9c8589192f1d31e011e99e58e6cd48fdb5843","abstract_canon_sha256":"7cf1f651ce65b0b66da2b45135ed715f07b525a59230812b34a4ba0ba1c3f17f"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:56:49.483865Z","signature_b64":"aI9EN5ikAon8XnMx7FpgpLGN9kyneICdINLm8iRu/BmfF6PyTSj+quk4aLNtO5ROCy1puJDLimvYXLIDgCu+CA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5482888a7e1adc00e3630285e646095b8348d19dfc3154629937b7843e032a59","last_reissued_at":"2026-05-17T23:56:49.483483Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:56:49.483483Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tunneling radiation of fermions from the non-stationary Kerr black hole","license":"http://creativecommons.org/licenses/by-sa/4.0/","headline":"","cross_cats":[],"primary_cat":"physics.gen-ph","authors_text":"Qun-Chao Ding, Shu-Zheng Yang, Zhong-Wen Feng","submitted_at":"2019-01-02T08:23:37Z","abstract_excerpt":"In this paper, the tunneling radiation of fermions with spin $1/2$ and $3/2$ from the non-stationary Kerr black hole are investigated. First, according to the Dirac equation for spin $1/2$ fermions and Rarita-Schwinger equation for spin $3/2$ fermions, we construct the corresponding gamma matrixes and the derive Hamilton-Jacobi equation for spin $1/2$ and $3/2$ fermions. Then, the tunneling behavior of fermions on the event horizon is studied. Finally, we obtain the thermodynamic properties of the non-stationary Kerr black hole. The result shows that the tunneling radiation rate, surface gravi"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.01852","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":"1901.01852","created_at":"2026-05-17T23:56:49.483541+00:00"},{"alias_kind":"arxiv_version","alias_value":"1901.01852v1","created_at":"2026-05-17T23:56:49.483541+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.01852","created_at":"2026-05-17T23:56:49.483541+00:00"},{"alias_kind":"pith_short_12","alias_value":"KSBIRCT6DLOA","created_at":"2026-05-18T12:33:21.387695+00:00"},{"alias_kind":"pith_short_16","alias_value":"KSBIRCT6DLOABY3D","created_at":"2026-05-18T12:33:21.387695+00:00"},{"alias_kind":"pith_short_8","alias_value":"KSBIRCT6","created_at":"2026-05-18T12:33:21.387695+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/KSBIRCT6DLOABY3DAKC6MRQJLO","json":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO.json","graph_json":"https://pith.science/api/pith-number/KSBIRCT6DLOABY3DAKC6MRQJLO/graph.json","events_json":"https://pith.science/api/pith-number/KSBIRCT6DLOABY3DAKC6MRQJLO/events.json","paper":"https://pith.science/paper/KSBIRCT6"},"agent_actions":{"view_html":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO","download_json":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO.json","view_paper":"https://pith.science/paper/KSBIRCT6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1901.01852&json=true","fetch_graph":"https://pith.science/api/pith-number/KSBIRCT6DLOABY3DAKC6MRQJLO/graph.json","fetch_events":"https://pith.science/api/pith-number/KSBIRCT6DLOABY3DAKC6MRQJLO/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO/action/storage_attestation","attest_author":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO/action/author_attestation","sign_citation":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO/action/citation_signature","submit_replication":"https://pith.science/pith/KSBIRCT6DLOABY3DAKC6MRQJLO/action/replication_record"}},"created_at":"2026-05-17T23:56:49.483541+00:00","updated_at":"2026-05-17T23:56:49.483541+00:00"}