{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:ZW5QLX5ASDGRAK4AOGPGNJMHLA","short_pith_number":"pith:ZW5QLX5A","schema_version":"1.0","canonical_sha256":"cdbb05dfa090cd102b80719e66a587582d1db0e8b0c7134d5ab1eeb97f9c41d0","source":{"kind":"arxiv","id":"1507.04172","version":2},"attestation_state":"computed","paper":{"title":"Gravitational anomalies and one dimensional behaviour of black holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Bibhas Ranjan Majhi","submitted_at":"2015-07-15T11:38:34Z","abstract_excerpt":"It has been pointed out by Bekenstein and Mayo that the behavior of the Black hole's entropy or information flow is similar to that through one-dimensional channel. Here I analyse the same issue with the use of gravitational anomalies. The rate of the entropy change ($\\dot{S}$) and the power ($P$) of the Hawking emission are calculated from the relevant components of the anomalous stress-tensor under the Unruh vacuum condition. I show that the dependence of $\\dot{S}$ on power is $\\dot{S}\\propto P^{1/2}$ which is identical to that for the information flow in one dimensional system. This is esta"},"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":"1507.04172","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2015-07-15T11:38:34Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b6b692a7d18591eb9c7acbe29c2f6b12452ecd6d981c18c2ff505feb2c9ba0a6","abstract_canon_sha256":"e810cb027aa2f967e4bdb6b744bfeae6081e43e29a9300a7f1b17c5c526564be"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:24:10.697856Z","signature_b64":"kFQiBxMhFoVgUegMQYI+AT50P5hOpcMY6fNPap5w8ACKGc8MSv1thrnazyPsPG+lVPQUNEoedm4pQ4QE8Z2hBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"cdbb05dfa090cd102b80719e66a587582d1db0e8b0c7134d5ab1eeb97f9c41d0","last_reissued_at":"2026-05-18T01:24:10.697408Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:24:10.697408Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitational anomalies and one dimensional behaviour of black holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"Bibhas Ranjan Majhi","submitted_at":"2015-07-15T11:38:34Z","abstract_excerpt":"It has been pointed out by Bekenstein and Mayo that the behavior of the Black hole's entropy or information flow is similar to that through one-dimensional channel. Here I analyse the same issue with the use of gravitational anomalies. The rate of the entropy change ($\\dot{S}$) and the power ($P$) of the Hawking emission are calculated from the relevant components of the anomalous stress-tensor under the Unruh vacuum condition. I show that the dependence of $\\dot{S}$ on power is $\\dot{S}\\propto P^{1/2}$ which is identical to that for the information flow in one dimensional system. This is esta"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1507.04172","kind":"arxiv","version":2},"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":"1507.04172","created_at":"2026-05-18T01:24:10.697489+00:00"},{"alias_kind":"arxiv_version","alias_value":"1507.04172v2","created_at":"2026-05-18T01:24:10.697489+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1507.04172","created_at":"2026-05-18T01:24:10.697489+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZW5QLX5ASDGR","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZW5QLX5ASDGRAK4A","created_at":"2026-05-18T12:29:52.810259+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZW5QLX5A","created_at":"2026-05-18T12:29:52.810259+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/ZW5QLX5ASDGRAK4AOGPGNJMHLA","json":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA.json","graph_json":"https://pith.science/api/pith-number/ZW5QLX5ASDGRAK4AOGPGNJMHLA/graph.json","events_json":"https://pith.science/api/pith-number/ZW5QLX5ASDGRAK4AOGPGNJMHLA/events.json","paper":"https://pith.science/paper/ZW5QLX5A"},"agent_actions":{"view_html":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA","download_json":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA.json","view_paper":"https://pith.science/paper/ZW5QLX5A","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1507.04172&json=true","fetch_graph":"https://pith.science/api/pith-number/ZW5QLX5ASDGRAK4AOGPGNJMHLA/graph.json","fetch_events":"https://pith.science/api/pith-number/ZW5QLX5ASDGRAK4AOGPGNJMHLA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA/action/storage_attestation","attest_author":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA/action/author_attestation","sign_citation":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA/action/citation_signature","submit_replication":"https://pith.science/pith/ZW5QLX5ASDGRAK4AOGPGNJMHLA/action/replication_record"}},"created_at":"2026-05-18T01:24:10.697489+00:00","updated_at":"2026-05-18T01:24:10.697489+00:00"}