{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:FUAYFDL5F7FKVO5FAEYILVS6LP","short_pith_number":"pith:FUAYFDL5","canonical_record":{"source":{"id":"1104.0356","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-04-03T05:29:50Z","cross_cats_sorted":[],"title_canon_sha256":"c22f329a5051849522f68a273fb8c76af15b4d4df8741da7135e672281c7b12f","abstract_canon_sha256":"72f8cc7b12b9670fd241a83012f2224965d26d8fa9bcb5d511997abaa1489a21"},"schema_version":"1.0"},"canonical_sha256":"2d01828d7d2fcaaabba5013085d65e5bfbc338606aa9a5001ca6475799a796f9","source":{"kind":"arxiv","id":"1104.0356","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.0356","created_at":"2026-05-18T02:02:41Z"},{"alias_kind":"arxiv_version","alias_value":"1104.0356v3","created_at":"2026-05-18T02:02:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.0356","created_at":"2026-05-18T02:02:41Z"},{"alias_kind":"pith_short_12","alias_value":"FUAYFDL5F7FK","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"FUAYFDL5F7FKVO5F","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"FUAYFDL5","created_at":"2026-05-18T12:26:28Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:FUAYFDL5F7FKVO5FAEYILVS6LP","target":"record","payload":{"canonical_record":{"source":{"id":"1104.0356","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-04-03T05:29:50Z","cross_cats_sorted":[],"title_canon_sha256":"c22f329a5051849522f68a273fb8c76af15b4d4df8741da7135e672281c7b12f","abstract_canon_sha256":"72f8cc7b12b9670fd241a83012f2224965d26d8fa9bcb5d511997abaa1489a21"},"schema_version":"1.0"},"canonical_sha256":"2d01828d7d2fcaaabba5013085d65e5bfbc338606aa9a5001ca6475799a796f9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:02:41.142415Z","signature_b64":"vYVHcgIkRwvYj4Gl8PZf5gWHHFFnBLE+h157IDsz9kn9IZAV8w523E6uIObPfu43kwT2iG8wVigo5k/gIZa+BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2d01828d7d2fcaaabba5013085d65e5bfbc338606aa9a5001ca6475799a796f9","last_reissued_at":"2026-05-18T02:02:41.141577Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:02:41.141577Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1104.0356","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:02:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Uel+SWD10qEXO1GAKKXqr6iIfAZNAPZuWTHcObl8HP5DDdS4ezkffP8ym+ZFyPQizrXz2m99sXsXxO8L72muCQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T09:35:37.276746Z"},"content_sha256":"6bd07c1ec30ed12680329c28c981c580f6c936ba9299f29ad69e343bd5c71903","schema_version":"1.0","event_id":"sha256:6bd07c1ec30ed12680329c28c981c580f6c936ba9299f29ad69e343bd5c71903"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:FUAYFDL5F7FKVO5FAEYILVS6LP","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Hawking Radiation for Scalar and Dirac Fields in Five Dimensional Dilatonic Black Hole via Anomalies","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"P. A. Gonz\\'alez, Ram\\'on Becar","submitted_at":"2011-04-03T05:29:50Z","abstract_excerpt":"We study massive scalar fields and Dirac fields propagating in a five dimensional dilatonic black hole background. We expose that for both fields the physics can be describe by a two dimensional theory, near the horizon. Then, in this limit, by applying the covariant anomalies method we find the Hawking flux by restoring the gauge invariance and the general coordinate covariance, which coincides with the flux obtained from integrating the Planck distribution for fermions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.0356","kind":"arxiv","version":3},"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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:02:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ZK5E6bPSsVSkXOb4Dfo/n/Dq/369lGUUCvxC51Kgp8ogNEX9yGDR+MmRhGcfnXFqI49vv0AVMYYdqN70PiT0CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T09:35:37.277371Z"},"content_sha256":"8843ee3f4d2e955178dae976ee1abfa643043b2f0e6cfc59e54f5418e23223ed","schema_version":"1.0","event_id":"sha256:8843ee3f4d2e955178dae976ee1abfa643043b2f0e6cfc59e54f5418e23223ed"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FUAYFDL5F7FKVO5FAEYILVS6LP/bundle.json","state_url":"https://pith.science/pith/FUAYFDL5F7FKVO5FAEYILVS6LP/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FUAYFDL5F7FKVO5FAEYILVS6LP/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-31T09:35:37Z","links":{"resolver":"https://pith.science/pith/FUAYFDL5F7FKVO5FAEYILVS6LP","bundle":"https://pith.science/pith/FUAYFDL5F7FKVO5FAEYILVS6LP/bundle.json","state":"https://pith.science/pith/FUAYFDL5F7FKVO5FAEYILVS6LP/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FUAYFDL5F7FKVO5FAEYILVS6LP/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:FUAYFDL5F7FKVO5FAEYILVS6LP","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"72f8cc7b12b9670fd241a83012f2224965d26d8fa9bcb5d511997abaa1489a21","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-04-03T05:29:50Z","title_canon_sha256":"c22f329a5051849522f68a273fb8c76af15b4d4df8741da7135e672281c7b12f"},"schema_version":"1.0","source":{"id":"1104.0356","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1104.0356","created_at":"2026-05-18T02:02:41Z"},{"alias_kind":"arxiv_version","alias_value":"1104.0356v3","created_at":"2026-05-18T02:02:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1104.0356","created_at":"2026-05-18T02:02:41Z"},{"alias_kind":"pith_short_12","alias_value":"FUAYFDL5F7FK","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_16","alias_value":"FUAYFDL5F7FKVO5F","created_at":"2026-05-18T12:26:28Z"},{"alias_kind":"pith_short_8","alias_value":"FUAYFDL5","created_at":"2026-05-18T12:26:28Z"}],"graph_snapshots":[{"event_id":"sha256:8843ee3f4d2e955178dae976ee1abfa643043b2f0e6cfc59e54f5418e23223ed","target":"graph","created_at":"2026-05-18T02:02:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We study massive scalar fields and Dirac fields propagating in a five dimensional dilatonic black hole background. We expose that for both fields the physics can be describe by a two dimensional theory, near the horizon. Then, in this limit, by applying the covariant anomalies method we find the Hawking flux by restoring the gauge invariance and the general coordinate covariance, which coincides with the flux obtained from integrating the Planck distribution for fermions.","authors_text":"P. A. Gonz\\'alez, Ram\\'on Becar","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-04-03T05:29:50Z","title":"Hawking Radiation for Scalar and Dirac Fields in Five Dimensional Dilatonic Black Hole via Anomalies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1104.0356","kind":"arxiv","version":3},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:6bd07c1ec30ed12680329c28c981c580f6c936ba9299f29ad69e343bd5c71903","target":"record","created_at":"2026-05-18T02:02:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"72f8cc7b12b9670fd241a83012f2224965d26d8fa9bcb5d511997abaa1489a21","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2011-04-03T05:29:50Z","title_canon_sha256":"c22f329a5051849522f68a273fb8c76af15b4d4df8741da7135e672281c7b12f"},"schema_version":"1.0","source":{"id":"1104.0356","kind":"arxiv","version":3}},"canonical_sha256":"2d01828d7d2fcaaabba5013085d65e5bfbc338606aa9a5001ca6475799a796f9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"2d01828d7d2fcaaabba5013085d65e5bfbc338606aa9a5001ca6475799a796f9","first_computed_at":"2026-05-18T02:02:41.141577Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:02:41.141577Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vYVHcgIkRwvYj4Gl8PZf5gWHHFFnBLE+h157IDsz9kn9IZAV8w523E6uIObPfu43kwT2iG8wVigo5k/gIZa+BQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:02:41.142415Z","signed_message":"canonical_sha256_bytes"},"source_id":"1104.0356","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:6bd07c1ec30ed12680329c28c981c580f6c936ba9299f29ad69e343bd5c71903","sha256:8843ee3f4d2e955178dae976ee1abfa643043b2f0e6cfc59e54f5418e23223ed"],"state_sha256":"39c9b56db8bb6881f3032160a32c2a00a10d0ada45f3b85bc48d49d3638910ed"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"idvIaCqUY52cORL9BH7WrmuU8DB6mo736IhlNa1aQPK0Kc5h7ZqnIqCDGRd3ztXcQGCMwJzq1SrrWChPmCgWCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T09:35:37.280412Z","bundle_sha256":"bf1eecb1e4b53a66c478a03efbcfdc931a427da89b6d275add320821e1c1cf29"}}