{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:3B2MXV2IZCQ7LOQ7B6RHWX62B3","short_pith_number":"pith:3B2MXV2I","canonical_record":{"source":{"id":"hep-th/0404166","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-04-22T09:03:49Z","cross_cats_sorted":["astro-ph","gr-qc"],"title_canon_sha256":"b1121ca41252c2d6f3353771041d9f79fcc4d0e3e14be06cfa55cefcced293a1","abstract_canon_sha256":"9f1a28ee79fdfcde6107816faa9c1077617b80d9f3a67196535a484dd1669997"},"schema_version":"1.0"},"canonical_sha256":"d874cbd748c8a1f5ba1f0fa27b5fda0ed983b3633909d3ae1dd7081d861566c0","source":{"kind":"arxiv","id":"hep-th/0404166","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0404166","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0404166v2","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0404166","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"pith_short_12","alias_value":"3B2MXV2IZCQ7","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"3B2MXV2IZCQ7LOQ7","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"3B2MXV2I","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:3B2MXV2IZCQ7LOQ7B6RHWX62B3","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0404166","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-04-22T09:03:49Z","cross_cats_sorted":["astro-ph","gr-qc"],"title_canon_sha256":"b1121ca41252c2d6f3353771041d9f79fcc4d0e3e14be06cfa55cefcced293a1","abstract_canon_sha256":"9f1a28ee79fdfcde6107816faa9c1077617b80d9f3a67196535a484dd1669997"},"schema_version":"1.0"},"canonical_sha256":"d874cbd748c8a1f5ba1f0fa27b5fda0ed983b3633909d3ae1dd7081d861566c0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:05:58.848618Z","signature_b64":"IhPHWYooJVeVrG94ujL9Xbc83DKoLBbyiFN/1Z40EYT4VeR0uaUeY6jTfF6Xliuww7pmKbo0yX2QsiUJOuTkAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d874cbd748c8a1f5ba1f0fa27b5fda0ed983b3633909d3ae1dd7081d861566c0","last_reissued_at":"2026-05-18T01:05:58.848099Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:05:58.848099Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0404166","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":"2026-05-18T01:05:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"rb4Uzurhqc21TpY4LL/zzMdKAE3Pt9/hkmpXo4F8yEDisfAGUHGG/YLgmtI/wx56hFwQraz9QrRE8bdjpq1bDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T04:05:08.372721Z"},"content_sha256":"5c91af6002622e5885ce65802ceb4dcb255150cd5242bc097881aabdd9ee3a6e","schema_version":"1.0","event_id":"sha256:5c91af6002622e5885ce65802ceb4dcb255150cd5242bc097881aabdd9ee3a6e"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:3B2MXV2IZCQ7LOQ7B6RHWX62B3","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Linearized gravity on the de Sitter brane in the Einstein Gauss-Bonnet theory","license":"","headline":"","cross_cats":["astro-ph","gr-qc"],"primary_cat":"hep-th","authors_text":"Masato Minamitsuji, Misao Sasaki","submitted_at":"2004-04-22T09:03:49Z","abstract_excerpt":"We investigate the linearized gravity on a single de Sitter brane in the anti-de Sitter (AdS) bulk in the Einstein Gauss-Bonnet (EGB) theory. We find that the Einstein gravity is recovered for a high energy brane, i.e., in the limit of the large expansion rate, $H\\ell\\gg 1$, where $H$ is the de Sitter expansion rate and $\\ell$ is the curvature radius of the AdS bulk.\n We also show that, in the short distance limit $r\\ll \\min\\{\\ell,H^{-1}\\}$, the Brans-Dicke gravity is obtained, whereas in the large distance limit $r\\gg\\max\\{\\ell,H^{-1}\\}$, the Brans-Dicke gravity is obtained for $H\\ell=O(1)$, "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0404166","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":"2026-05-18T01:05:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"IGNcjuTkCO49/v5WMfCuuGv0zoMn/DV0O2nwTgUCWIZAmns9i7vTy5X6D+nEPG/rlfwvvH0v5j4HclQXPyclCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T04:05:08.373135Z"},"content_sha256":"8972f3a32ffe41fb11702c53861cf60522ecb35b080fa4f231ed6e56d7fbbdb4","schema_version":"1.0","event_id":"sha256:8972f3a32ffe41fb11702c53861cf60522ecb35b080fa4f231ed6e56d7fbbdb4"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3B2MXV2IZCQ7LOQ7B6RHWX62B3/bundle.json","state_url":"https://pith.science/pith/3B2MXV2IZCQ7LOQ7B6RHWX62B3/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3B2MXV2IZCQ7LOQ7B6RHWX62B3/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":"2026-05-28T04:05:08Z","links":{"resolver":"https://pith.science/pith/3B2MXV2IZCQ7LOQ7B6RHWX62B3","bundle":"https://pith.science/pith/3B2MXV2IZCQ7LOQ7B6RHWX62B3/bundle.json","state":"https://pith.science/pith/3B2MXV2IZCQ7LOQ7B6RHWX62B3/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3B2MXV2IZCQ7LOQ7B6RHWX62B3/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:3B2MXV2IZCQ7LOQ7B6RHWX62B3","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":"9f1a28ee79fdfcde6107816faa9c1077617b80d9f3a67196535a484dd1669997","cross_cats_sorted":["astro-ph","gr-qc"],"license":"","primary_cat":"hep-th","submitted_at":"2004-04-22T09:03:49Z","title_canon_sha256":"b1121ca41252c2d6f3353771041d9f79fcc4d0e3e14be06cfa55cefcced293a1"},"schema_version":"1.0","source":{"id":"hep-th/0404166","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0404166","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0404166v2","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0404166","created_at":"2026-05-18T01:05:58Z"},{"alias_kind":"pith_short_12","alias_value":"3B2MXV2IZCQ7","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"3B2MXV2IZCQ7LOQ7","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"3B2MXV2I","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:8972f3a32ffe41fb11702c53861cf60522ecb35b080fa4f231ed6e56d7fbbdb4","target":"graph","created_at":"2026-05-18T01:05:58Z","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 investigate the linearized gravity on a single de Sitter brane in the anti-de Sitter (AdS) bulk in the Einstein Gauss-Bonnet (EGB) theory. We find that the Einstein gravity is recovered for a high energy brane, i.e., in the limit of the large expansion rate, $H\\ell\\gg 1$, where $H$ is the de Sitter expansion rate and $\\ell$ is the curvature radius of the AdS bulk.\n We also show that, in the short distance limit $r\\ll \\min\\{\\ell,H^{-1}\\}$, the Brans-Dicke gravity is obtained, whereas in the large distance limit $r\\gg\\max\\{\\ell,H^{-1}\\}$, the Brans-Dicke gravity is obtained for $H\\ell=O(1)$, ","authors_text":"Masato Minamitsuji, Misao Sasaki","cross_cats":["astro-ph","gr-qc"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2004-04-22T09:03:49Z","title":"Linearized gravity on the de Sitter brane in the Einstein Gauss-Bonnet theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0404166","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":"sha256:5c91af6002622e5885ce65802ceb4dcb255150cd5242bc097881aabdd9ee3a6e","target":"record","created_at":"2026-05-18T01:05:58Z","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":"9f1a28ee79fdfcde6107816faa9c1077617b80d9f3a67196535a484dd1669997","cross_cats_sorted":["astro-ph","gr-qc"],"license":"","primary_cat":"hep-th","submitted_at":"2004-04-22T09:03:49Z","title_canon_sha256":"b1121ca41252c2d6f3353771041d9f79fcc4d0e3e14be06cfa55cefcced293a1"},"schema_version":"1.0","source":{"id":"hep-th/0404166","kind":"arxiv","version":2}},"canonical_sha256":"d874cbd748c8a1f5ba1f0fa27b5fda0ed983b3633909d3ae1dd7081d861566c0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d874cbd748c8a1f5ba1f0fa27b5fda0ed983b3633909d3ae1dd7081d861566c0","first_computed_at":"2026-05-18T01:05:58.848099Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:05:58.848099Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"IhPHWYooJVeVrG94ujL9Xbc83DKoLBbyiFN/1Z40EYT4VeR0uaUeY6jTfF6Xliuww7pmKbo0yX2QsiUJOuTkAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:05:58.848618Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0404166","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5c91af6002622e5885ce65802ceb4dcb255150cd5242bc097881aabdd9ee3a6e","sha256:8972f3a32ffe41fb11702c53861cf60522ecb35b080fa4f231ed6e56d7fbbdb4"],"state_sha256":"9cc12710c3bb13d3a3a83774acfe91288af4fc30ec3ad1c4e365f3b8e90f7ca4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"tBzHfr5/mnVM76Mzt76tBQ1FSwyinE0mKUwhPdvkrFuru36EkXhCR45E8g6C99CBs2NNacbH8shKpveifU9yAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T04:05:08.375235Z","bundle_sha256":"2573194d00f08b2e7340b864115035cc954be870272c138cb112ce81cea9f0de"}}