{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:QATQR4YOBRPMJOM7NKNIBZABS3","short_pith_number":"pith:QATQR4YO","schema_version":"1.0","canonical_sha256":"802708f30e0c5ec4b99f6a9a80e40196e8037286d8598d6813c1a1acc59582bd","source":{"kind":"arxiv","id":"gr-qc/0403002","version":4},"attestation_state":"computed","paper":{"title":"Rotating black holes in brane worlds","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Dejan Stojkovic, Dmitri V. Fursaev, Valeri P. Frolov","submitted_at":"2004-02-27T23:09:21Z","abstract_excerpt":"We study interaction of rotating higher dimensional black holes with a brane in space-times with large extra dimensions. We demonstrate that a rotating black hole attached to a brane can be stationary only if the null Killing vector generating the black hole horizon is tangent to the brane world-sheet. The characteristic time when a rotating black hole with the gravitational radius $r_0$ reaches this final stationary state is $T\\sim r_0^{p-1}/(G\\sigma)$, where $G$ is the higher dimensional gravitational coupling constant, $\\sigma$ is the brane tension, and $p$ is the number of extra dimensions"},"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":"gr-qc/0403002","kind":"arxiv","version":4},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"2004-02-27T23:09:21Z","cross_cats_sorted":[],"title_canon_sha256":"dc893b9b96bdbb95beca844100dd24932f0eb608e05b6aee1e9cdaa8c55343d4","abstract_canon_sha256":"d3490603e37f3d9772031aa32ce2063855201b5f4a362873746f730ad74598a4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:47:41.964504Z","signature_b64":"2jZRP7RNX400TtrvOL+Kqv+uM145UHHLnHk9H3/K9Vf3iin7x7oCPP+sDsj9pbUGjE+vvAO073wu4hHUWAaxBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"802708f30e0c5ec4b99f6a9a80e40196e8037286d8598d6813c1a1acc59582bd","last_reissued_at":"2026-07-04T16:47:41.964153Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:47:41.964153Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Rotating black holes in brane worlds","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Dejan Stojkovic, Dmitri V. Fursaev, Valeri P. Frolov","submitted_at":"2004-02-27T23:09:21Z","abstract_excerpt":"We study interaction of rotating higher dimensional black holes with a brane in space-times with large extra dimensions. We demonstrate that a rotating black hole attached to a brane can be stationary only if the null Killing vector generating the black hole horizon is tangent to the brane world-sheet. The characteristic time when a rotating black hole with the gravitational radius $r_0$ reaches this final stationary state is $T\\sim r_0^{p-1}/(G\\sigma)$, where $G$ is the higher dimensional gravitational coupling constant, $\\sigma$ is the brane tension, and $p$ is the number of extra dimensions"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/0403002","kind":"arxiv","version":4},"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/gr-qc/0403002/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":"gr-qc/0403002","created_at":"2026-07-04T16:47:41.964215+00:00"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/0403002v4","created_at":"2026-07-04T16:47:41.964215+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/0403002","created_at":"2026-07-04T16:47:41.964215+00:00"},{"alias_kind":"pith_short_12","alias_value":"QATQR4YOBRPM","created_at":"2026-07-04T16:47:41.964215+00:00"},{"alias_kind":"pith_short_16","alias_value":"QATQR4YOBRPMJOM7","created_at":"2026-07-04T16:47:41.964215+00:00"},{"alias_kind":"pith_short_8","alias_value":"QATQR4YO","created_at":"2026-07-04T16:47:41.964215+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/QATQR4YOBRPMJOM7NKNIBZABS3","json":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3.json","graph_json":"https://pith.science/api/pith-number/QATQR4YOBRPMJOM7NKNIBZABS3/graph.json","events_json":"https://pith.science/api/pith-number/QATQR4YOBRPMJOM7NKNIBZABS3/events.json","paper":"https://pith.science/paper/QATQR4YO"},"agent_actions":{"view_html":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3","download_json":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3.json","view_paper":"https://pith.science/paper/QATQR4YO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=gr-qc/0403002&json=true","fetch_graph":"https://pith.science/api/pith-number/QATQR4YOBRPMJOM7NKNIBZABS3/graph.json","fetch_events":"https://pith.science/api/pith-number/QATQR4YOBRPMJOM7NKNIBZABS3/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3/action/timestamp_anchor","attest_storage":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3/action/storage_attestation","attest_author":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3/action/author_attestation","sign_citation":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3/action/citation_signature","submit_replication":"https://pith.science/pith/QATQR4YOBRPMJOM7NKNIBZABS3/action/replication_record"}},"created_at":"2026-07-04T16:47:41.964215+00:00","updated_at":"2026-07-04T16:47:41.964215+00:00"}