{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:NCA3TOUCOB373W42OJ4Y4NBH4H","short_pith_number":"pith:NCA3TOUC","canonical_record":{"source":{"id":"hep-ph/0212199","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-12-13T20:46:57Z","cross_cats_sorted":["astro-ph","gr-qc","hep-th"],"title_canon_sha256":"d6fe0db5ce80e77a6330c6194d6a10fdb97c94aecf2f9fe5076d8744b7d0351d","abstract_canon_sha256":"af3f125a6e7f46820bbfb212f012ffc41626af0beca7d270815eb24da7887277"},"schema_version":"1.0"},"canonical_sha256":"6881b9ba827077fddb9a72798e3427e1fd5e195b45113203d4f2a0cade0f34f9","source":{"kind":"arxiv","id":"hep-ph/0212199","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0212199","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0212199v3","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0212199","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"pith_short_12","alias_value":"NCA3TOUCOB37","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"pith_short_16","alias_value":"NCA3TOUCOB373W42","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"pith_short_8","alias_value":"NCA3TOUC","created_at":"2026-07-04T15:20:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:NCA3TOUCOB373W42OJ4Y4NBH4H","target":"record","payload":{"canonical_record":{"source":{"id":"hep-ph/0212199","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2002-12-13T20:46:57Z","cross_cats_sorted":["astro-ph","gr-qc","hep-th"],"title_canon_sha256":"d6fe0db5ce80e77a6330c6194d6a10fdb97c94aecf2f9fe5076d8744b7d0351d","abstract_canon_sha256":"af3f125a6e7f46820bbfb212f012ffc41626af0beca7d270815eb24da7887277"},"schema_version":"1.0"},"canonical_sha256":"6881b9ba827077fddb9a72798e3427e1fd5e195b45113203d4f2a0cade0f34f9","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:20:20.504911Z","signature_b64":"ISuI35LsO5HQ3Uo/G7zjlsS7N8OPvWkxOhHb3vIuxG7FwEs4NBQ2CltppIFK8pNqiqz+d7MXQF3YQejwzpJaAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6881b9ba827077fddb9a72798e3427e1fd5e195b45113203d4f2a0cade0f34f9","last_reissued_at":"2026-07-04T15:20:20.504483Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:20:20.504483Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-ph/0212199","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":"2026-07-04T15:20:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Ei88lbhj2BJR1ef70fnzdELn/DxcXkSEzzJ7VXWkhfoRm6JPvsP0FAOcwIq2jOVJxV9W8WOQO74Kwg/nNR3NAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T21:19:17.104983Z"},"content_sha256":"cc6ae6189af6531e0c7a75df09773fac390ff01d75093aec77182789ff2675ec","schema_version":"1.0","event_id":"sha256:cc6ae6189af6531e0c7a75df09773fac390ff01d75093aec77182789ff2675ec"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:NCA3TOUCOB373W42OJ4Y4NBH4H","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Calculable Corrections to Brane Black Hole Decay II: Greybody Factors for Spin 1/2 and 1","license":"","headline":"","cross_cats":["astro-ph","gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"John March-Russell, Panagiota Kanti","submitted_at":"2002-12-13T20:46:57Z","abstract_excerpt":"The production of black holes in extra-dimensional brane-world theories can lead to detectable signals via the Hawking evaporation of the black hole to brane-localised Standard Model modes. We calculate, as a function of partial wave number and number of toroidally compactified extra dimensions, the leading correction to the energy spectrum of such Hawking radiation (the greybody factors) for decay into spin 1/2 fermions and spin 1 gauge fields localised on the Standard Model brane. We derive the associated improved differential emission rates for both types of fields. We provide both simple e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0212199","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0212199/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T15:20:20Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"qQXmoFqlf41LcENxrJFF8Fybqm305vcb+Y7HziFqIPen25RMgaDhzwdzGsmApvDECOI6chH3SKC32DZfkaHzBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-15T21:19:17.105712Z"},"content_sha256":"1d6c48ba85180832e870d29d0d9c710059daa7ff318134c89701e81a22f8cc8b","schema_version":"1.0","event_id":"sha256:1d6c48ba85180832e870d29d0d9c710059daa7ff318134c89701e81a22f8cc8b"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/NCA3TOUCOB373W42OJ4Y4NBH4H/bundle.json","state_url":"https://pith.science/pith/NCA3TOUCOB373W42OJ4Y4NBH4H/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/NCA3TOUCOB373W42OJ4Y4NBH4H/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":"2026-08-15T21:19:17Z","links":{"resolver":"https://pith.science/pith/NCA3TOUCOB373W42OJ4Y4NBH4H","bundle":"https://pith.science/pith/NCA3TOUCOB373W42OJ4Y4NBH4H/bundle.json","state":"https://pith.science/pith/NCA3TOUCOB373W42OJ4Y4NBH4H/state.json","well_known_bundle":"https://pith.science/.well-known/pith/NCA3TOUCOB373W42OJ4Y4NBH4H/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:NCA3TOUCOB373W42OJ4Y4NBH4H","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":"af3f125a6e7f46820bbfb212f012ffc41626af0beca7d270815eb24da7887277","cross_cats_sorted":["astro-ph","gr-qc","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2002-12-13T20:46:57Z","title_canon_sha256":"d6fe0db5ce80e77a6330c6194d6a10fdb97c94aecf2f9fe5076d8744b7d0351d"},"schema_version":"1.0","source":{"id":"hep-ph/0212199","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-ph/0212199","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0212199v3","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0212199","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"pith_short_12","alias_value":"NCA3TOUCOB37","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"pith_short_16","alias_value":"NCA3TOUCOB373W42","created_at":"2026-07-04T15:20:20Z"},{"alias_kind":"pith_short_8","alias_value":"NCA3TOUC","created_at":"2026-07-04T15:20:20Z"}],"graph_snapshots":[{"event_id":"sha256:1d6c48ba85180832e870d29d0d9c710059daa7ff318134c89701e81a22f8cc8b","target":"graph","created_at":"2026-07-04T15:20:20Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/hep-ph/0212199/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The production of black holes in extra-dimensional brane-world theories can lead to detectable signals via the Hawking evaporation of the black hole to brane-localised Standard Model modes. We calculate, as a function of partial wave number and number of toroidally compactified extra dimensions, the leading correction to the energy spectrum of such Hawking radiation (the greybody factors) for decay into spin 1/2 fermions and spin 1 gauge fields localised on the Standard Model brane. We derive the associated improved differential emission rates for both types of fields. We provide both simple e","authors_text":"John March-Russell, Panagiota Kanti","cross_cats":["astro-ph","gr-qc","hep-th"],"headline":"","license":"","primary_cat":"hep-ph","submitted_at":"2002-12-13T20:46:57Z","title":"Calculable Corrections to Brane Black Hole Decay II: Greybody Factors for Spin 1/2 and 1"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0212199","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:cc6ae6189af6531e0c7a75df09773fac390ff01d75093aec77182789ff2675ec","target":"record","created_at":"2026-07-04T15:20:20Z","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":"af3f125a6e7f46820bbfb212f012ffc41626af0beca7d270815eb24da7887277","cross_cats_sorted":["astro-ph","gr-qc","hep-th"],"license":"","primary_cat":"hep-ph","submitted_at":"2002-12-13T20:46:57Z","title_canon_sha256":"d6fe0db5ce80e77a6330c6194d6a10fdb97c94aecf2f9fe5076d8744b7d0351d"},"schema_version":"1.0","source":{"id":"hep-ph/0212199","kind":"arxiv","version":3}},"canonical_sha256":"6881b9ba827077fddb9a72798e3427e1fd5e195b45113203d4f2a0cade0f34f9","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"6881b9ba827077fddb9a72798e3427e1fd5e195b45113203d4f2a0cade0f34f9","first_computed_at":"2026-07-04T15:20:20.504483Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:20:20.504483Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"ISuI35LsO5HQ3Uo/G7zjlsS7N8OPvWkxOhHb3vIuxG7FwEs4NBQ2CltppIFK8pNqiqz+d7MXQF3YQejwzpJaAw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:20:20.504911Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-ph/0212199","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cc6ae6189af6531e0c7a75df09773fac390ff01d75093aec77182789ff2675ec","sha256:1d6c48ba85180832e870d29d0d9c710059daa7ff318134c89701e81a22f8cc8b"],"state_sha256":"b0ac5ec77239a4873b018098cec088e2aaa710dbe9d2c238e10bca4e78cd4494"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"1FNSrys57tZvcEiNuF1ZZQnZZY6+ysvlvdRUVcyYy1V11dugN0GvE8bqHCuFKCo9+9ED/XG5ONQOvau7Jw+TAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-15T21:19:17.111766Z","bundle_sha256":"1c3356f769bd5dcba5c575ef009afa36fb80f53e61af9cb29d5437df4ac93ccc"}}