{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:4HLUZORLV3BLULOWGSYF4TZMML","short_pith_number":"pith:4HLUZORL","canonical_record":{"source":{"id":"1110.5651","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-ph","submitted_at":"2011-10-25T20:02:50Z","cross_cats_sorted":[],"title_canon_sha256":"bed2cc0b4e0434be18d5660a9d4d614f00a641bd59c4badf9b19a4b1d5e5f97a","abstract_canon_sha256":"015d4d14b0ccbdd3017d051c03b4553dd05539fb3445966505e4cafc7b93105c"},"schema_version":"1.0"},"canonical_sha256":"e1d74cba2baec2ba2dd634b05e4f2c62ca77589954d9192f997cf37e9c7a2d02","source":{"kind":"arxiv","id":"1110.5651","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.5651","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"arxiv_version","alias_value":"1110.5651v2","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.5651","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"pith_short_12","alias_value":"4HLUZORLV3BL","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4HLUZORLV3BLULOW","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4HLUZORL","created_at":"2026-05-18T12:26:20Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:4HLUZORLV3BLULOWGSYF4TZMML","target":"record","payload":{"canonical_record":{"source":{"id":"1110.5651","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-ph","submitted_at":"2011-10-25T20:02:50Z","cross_cats_sorted":[],"title_canon_sha256":"bed2cc0b4e0434be18d5660a9d4d614f00a641bd59c4badf9b19a4b1d5e5f97a","abstract_canon_sha256":"015d4d14b0ccbdd3017d051c03b4553dd05539fb3445966505e4cafc7b93105c"},"schema_version":"1.0"},"canonical_sha256":"e1d74cba2baec2ba2dd634b05e4f2c62ca77589954d9192f997cf37e9c7a2d02","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:00:15.598284Z","signature_b64":"zP8aORYwJy2d6srj0gYy0F6avpHw55HU8ygpotmZDExYv9jbBRuktSC59q7cNcarHZMJrMLGJKQmfUVGC4o8AQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e1d74cba2baec2ba2dd634b05e4f2c62ca77589954d9192f997cf37e9c7a2d02","last_reissued_at":"2026-05-18T04:00:15.597578Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:00:15.597578Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1110.5651","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:00:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rtVCS3IJynFVFvIZ7sCUP+ddKSwewawkwwGxcVpY11DXc73x+6g5RajXUxjy/lxwOHOtGcHZRxERryRkwF5bDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T13:53:14.469106Z"},"content_sha256":"5864e32569dacab48a7277ed67ecb3dcfecf54cf7dcc04cd09dd227c07615b0b","schema_version":"1.0","event_id":"sha256:5864e32569dacab48a7277ed67ecb3dcfecf54cf7dcc04cd09dd227c07615b0b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:4HLUZORLV3BLULOWGSYF4TZMML","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Effective Lagrangian for Bulk Fermions in Models with Extra Dimensions","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Adrian Carmona, Jose Santiago","submitted_at":"2011-10-25T20:02:50Z","abstract_excerpt":"We compute the dimension 6 effective Lagrangian arising from the tree level integration of an arbitrary number of bulk fermions in models with warped extra dimensions. The coefficients of the effective operators are written in terms of simple integrals of the metric and are valid for arbitrary warp factors, with or without an infrared brane, and for a general Higgs profile. All relevant tree level fermion effects in electroweak and flavor observables can be computed using this effective Lagrangian."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.5651","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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T04:00:15Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"MuxhT0xcKJ34le2q+oBdJOwLroy4c+K+eeXIwv/F0t82cttB2suv1HF/50ApCrc5NSO6TbFAKZ7G/InYnqSRAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-26T13:53:14.469766Z"},"content_sha256":"8544dfa97493c48f3b70b54edbd35324d1a7365726b8569990223f34337b5cbb","schema_version":"1.0","event_id":"sha256:8544dfa97493c48f3b70b54edbd35324d1a7365726b8569990223f34337b5cbb"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/4HLUZORLV3BLULOWGSYF4TZMML/bundle.json","state_url":"https://pith.science/pith/4HLUZORLV3BLULOWGSYF4TZMML/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/4HLUZORLV3BLULOWGSYF4TZMML/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":"2026-05-26T13:53:14Z","links":{"resolver":"https://pith.science/pith/4HLUZORLV3BLULOWGSYF4TZMML","bundle":"https://pith.science/pith/4HLUZORLV3BLULOWGSYF4TZMML/bundle.json","state":"https://pith.science/pith/4HLUZORLV3BLULOWGSYF4TZMML/state.json","well_known_bundle":"https://pith.science/.well-known/pith/4HLUZORLV3BLULOWGSYF4TZMML/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:4HLUZORLV3BLULOWGSYF4TZMML","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":"015d4d14b0ccbdd3017d051c03b4553dd05539fb3445966505e4cafc7b93105c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-ph","submitted_at":"2011-10-25T20:02:50Z","title_canon_sha256":"bed2cc0b4e0434be18d5660a9d4d614f00a641bd59c4badf9b19a4b1d5e5f97a"},"schema_version":"1.0","source":{"id":"1110.5651","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1110.5651","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"arxiv_version","alias_value":"1110.5651v2","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1110.5651","created_at":"2026-05-18T04:00:15Z"},{"alias_kind":"pith_short_12","alias_value":"4HLUZORLV3BL","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_16","alias_value":"4HLUZORLV3BLULOW","created_at":"2026-05-18T12:26:20Z"},{"alias_kind":"pith_short_8","alias_value":"4HLUZORL","created_at":"2026-05-18T12:26:20Z"}],"graph_snapshots":[{"event_id":"sha256:8544dfa97493c48f3b70b54edbd35324d1a7365726b8569990223f34337b5cbb","target":"graph","created_at":"2026-05-18T04:00:15Z","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 compute the dimension 6 effective Lagrangian arising from the tree level integration of an arbitrary number of bulk fermions in models with warped extra dimensions. The coefficients of the effective operators are written in terms of simple integrals of the metric and are valid for arbitrary warp factors, with or without an infrared brane, and for a general Higgs profile. All relevant tree level fermion effects in electroweak and flavor observables can be computed using this effective Lagrangian.","authors_text":"Adrian Carmona, Jose Santiago","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-ph","submitted_at":"2011-10-25T20:02:50Z","title":"The Effective Lagrangian for Bulk Fermions in Models with Extra Dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1110.5651","kind":"arxiv","version":2},"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":"sha256:5864e32569dacab48a7277ed67ecb3dcfecf54cf7dcc04cd09dd227c07615b0b","target":"record","created_at":"2026-05-18T04:00:15Z","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":"015d4d14b0ccbdd3017d051c03b4553dd05539fb3445966505e4cafc7b93105c","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by-nc-sa/3.0/","primary_cat":"hep-ph","submitted_at":"2011-10-25T20:02:50Z","title_canon_sha256":"bed2cc0b4e0434be18d5660a9d4d614f00a641bd59c4badf9b19a4b1d5e5f97a"},"schema_version":"1.0","source":{"id":"1110.5651","kind":"arxiv","version":2}},"canonical_sha256":"e1d74cba2baec2ba2dd634b05e4f2c62ca77589954d9192f997cf37e9c7a2d02","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e1d74cba2baec2ba2dd634b05e4f2c62ca77589954d9192f997cf37e9c7a2d02","first_computed_at":"2026-05-18T04:00:15.597578Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:00:15.597578Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"zP8aORYwJy2d6srj0gYy0F6avpHw55HU8ygpotmZDExYv9jbBRuktSC59q7cNcarHZMJrMLGJKQmfUVGC4o8AQ==","signature_status":"signed_v1","signed_at":"2026-05-18T04:00:15.598284Z","signed_message":"canonical_sha256_bytes"},"source_id":"1110.5651","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5864e32569dacab48a7277ed67ecb3dcfecf54cf7dcc04cd09dd227c07615b0b","sha256:8544dfa97493c48f3b70b54edbd35324d1a7365726b8569990223f34337b5cbb"],"state_sha256":"752540edb601149d05727362283e241df385fe1f44d73849132f713a012593ea"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/ciJaix8zFoR16N8BadvkLAnvZHniqqBhSn+5HeM5Ll/f3M+2dWUtSb4Ba0j+IwG78RduIbrxRNvvok3OYGxCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-26T13:53:14.473204Z","bundle_sha256":"c1cd132d62e9774a275b93653afedc76f6290d4f77dd1d4ac3f08caf1dcbe9d0"}}