{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2022:TYAA2QSRTDOXY5TC5L7OYAAAE5","short_pith_number":"pith:TYAA2QSR","canonical_record":{"source":{"id":"2205.10600","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-21T14:02:12Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"0914502d80b5d69b1cd962c30ddc4d0b29399701f1cde92e1e649c636aa90f70","abstract_canon_sha256":"190b8f55f2294fc78000008b05c41cd668d4837e30e3bac25485335b7a357715"},"schema_version":"1.0"},"canonical_sha256":"9e000d425198dd7c7662eafeec0000277a56534499b69976a4127b4e7dc62df0","source":{"kind":"arxiv","id":"2205.10600","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.10600","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"arxiv_version","alias_value":"2205.10600v2","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.10600","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"pith_short_12","alias_value":"TYAA2QSRTDOX","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"pith_short_16","alias_value":"TYAA2QSRTDOXY5TC","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"pith_short_8","alias_value":"TYAA2QSR","created_at":"2026-07-05T05:01:23Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2022:TYAA2QSRTDOXY5TC5L7OYAAAE5","target":"record","payload":{"canonical_record":{"source":{"id":"2205.10600","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-21T14:02:12Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"0914502d80b5d69b1cd962c30ddc4d0b29399701f1cde92e1e649c636aa90f70","abstract_canon_sha256":"190b8f55f2294fc78000008b05c41cd668d4837e30e3bac25485335b7a357715"},"schema_version":"1.0"},"canonical_sha256":"9e000d425198dd7c7662eafeec0000277a56534499b69976a4127b4e7dc62df0","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:01:23.508867Z","signature_b64":"VBFUsrjGMGD5nKLlWMMdyViMfU3Y4xAXioy6fEAO15tsIgT78thdGrXaB4Zm3aaAV+idQGINFRZhzF499XG6Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e000d425198dd7c7662eafeec0000277a56534499b69976a4127b4e7dc62df0","last_reissued_at":"2026-07-05T05:01:23.508438Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:01:23.508438Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2205.10600","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":"2026-07-05T05:01:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9oxIrDvl0GPEYvzlE/mQnw0IQXLVVXHGUb86/MOSaFHyiFq/Leov5jSs97XOR8aUXBznx9+wnfgY5bbA1HglDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T21:16:33.693543Z"},"content_sha256":"9d23318692587a14eae070958bc9710d8a010a2b23acb6c56791983251d1f335","schema_version":"1.0","event_id":"sha256:9d23318692587a14eae070958bc9710d8a010a2b23acb6c56791983251d1f335"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2022:TYAA2QSRTDOXY5TC5L7OYAAAE5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the Dynamics in the AdS/BCFT Correspondence","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-th","authors_text":"Seiji Terashima, Yu-ki Suzuki","submitted_at":"2022-05-21T14:02:12Z","abstract_excerpt":"We consider a perturbation of the Einstein gravity with the Neumann boundary condition, which is regarded as an end of the world brane (ETW brane) of the AdS/BCFT correspondence, in the AdSd+1 spaectime where d is larger than 2. We obtain the mode expansion of the perturbations explicitly for the tensionless ETW brane case. We also show that the energy-momentum tensor in a d-dimensional BCFT should satisfy nontrivial constraints other than the ones for the boundary conformal symmetry if the BCFT can couple to a d-dimensional gravity with a specific boundary condition, which can be the Neumann "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.10600","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2205.10600/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":"2026-07-05T05:01:23Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kuAlFT8eN7Y8iWJRyXptWptaKxhhAHyY2M54Anyk05IP7rf3Etz8UnQwboJRgZGiJDTE77qQAgne52OF5IsTBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-10T21:16:33.694435Z"},"content_sha256":"c8c566242c76f8fb5abc7e8c85168460106dd043bcf71930abe33641857b7192","schema_version":"1.0","event_id":"sha256:c8c566242c76f8fb5abc7e8c85168460106dd043bcf71930abe33641857b7192"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/TYAA2QSRTDOXY5TC5L7OYAAAE5/bundle.json","state_url":"https://pith.science/pith/TYAA2QSRTDOXY5TC5L7OYAAAE5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/TYAA2QSRTDOXY5TC5L7OYAAAE5/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":"2026-08-10T21:16:33Z","links":{"resolver":"https://pith.science/pith/TYAA2QSRTDOXY5TC5L7OYAAAE5","bundle":"https://pith.science/pith/TYAA2QSRTDOXY5TC5L7OYAAAE5/bundle.json","state":"https://pith.science/pith/TYAA2QSRTDOXY5TC5L7OYAAAE5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/TYAA2QSRTDOXY5TC5L7OYAAAE5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:TYAA2QSRTDOXY5TC5L7OYAAAE5","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":"190b8f55f2294fc78000008b05c41cd668d4837e30e3bac25485335b7a357715","cross_cats_sorted":["gr-qc"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-21T14:02:12Z","title_canon_sha256":"0914502d80b5d69b1cd962c30ddc4d0b29399701f1cde92e1e649c636aa90f70"},"schema_version":"1.0","source":{"id":"2205.10600","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2205.10600","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"arxiv_version","alias_value":"2205.10600v2","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2205.10600","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"pith_short_12","alias_value":"TYAA2QSRTDOX","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"pith_short_16","alias_value":"TYAA2QSRTDOXY5TC","created_at":"2026-07-05T05:01:23Z"},{"alias_kind":"pith_short_8","alias_value":"TYAA2QSR","created_at":"2026-07-05T05:01:23Z"}],"graph_snapshots":[{"event_id":"sha256:c8c566242c76f8fb5abc7e8c85168460106dd043bcf71930abe33641857b7192","target":"graph","created_at":"2026-07-05T05:01:23Z","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/2205.10600/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We consider a perturbation of the Einstein gravity with the Neumann boundary condition, which is regarded as an end of the world brane (ETW brane) of the AdS/BCFT correspondence, in the AdSd+1 spaectime where d is larger than 2. We obtain the mode expansion of the perturbations explicitly for the tensionless ETW brane case. We also show that the energy-momentum tensor in a d-dimensional BCFT should satisfy nontrivial constraints other than the ones for the boundary conformal symmetry if the BCFT can couple to a d-dimensional gravity with a specific boundary condition, which can be the Neumann ","authors_text":"Seiji Terashima, Yu-ki Suzuki","cross_cats":["gr-qc"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-21T14:02:12Z","title":"On the Dynamics in the AdS/BCFT Correspondence"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2205.10600","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":"sha256:9d23318692587a14eae070958bc9710d8a010a2b23acb6c56791983251d1f335","target":"record","created_at":"2026-07-05T05:01:23Z","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":"190b8f55f2294fc78000008b05c41cd668d4837e30e3bac25485335b7a357715","cross_cats_sorted":["gr-qc"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-th","submitted_at":"2022-05-21T14:02:12Z","title_canon_sha256":"0914502d80b5d69b1cd962c30ddc4d0b29399701f1cde92e1e649c636aa90f70"},"schema_version":"1.0","source":{"id":"2205.10600","kind":"arxiv","version":2}},"canonical_sha256":"9e000d425198dd7c7662eafeec0000277a56534499b69976a4127b4e7dc62df0","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9e000d425198dd7c7662eafeec0000277a56534499b69976a4127b4e7dc62df0","first_computed_at":"2026-07-05T05:01:23.508438Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:01:23.508438Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"VBFUsrjGMGD5nKLlWMMdyViMfU3Y4xAXioy6fEAO15tsIgT78thdGrXaB4Zm3aaAV+idQGINFRZhzF499XG6Ag==","signature_status":"signed_v1","signed_at":"2026-07-05T05:01:23.508867Z","signed_message":"canonical_sha256_bytes"},"source_id":"2205.10600","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:9d23318692587a14eae070958bc9710d8a010a2b23acb6c56791983251d1f335","sha256:c8c566242c76f8fb5abc7e8c85168460106dd043bcf71930abe33641857b7192"],"state_sha256":"93e7c46b3fa878d7d9dc24ce8d29837ec2cf8fedefaa1b8996956748c68b4cba"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"ubRSLpb1VDddX0zX6cEpEhD7rtD9ecCVpMpFUt+Rtj7NGBS2ZIXUMmbDmpb9poGTo2D/95QQaa+GVCAe++xiCQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-10T21:16:33.701373Z","bundle_sha256":"65e7d1b416d9d8fb1dd72f0256a278ca76a530b0ae1792a833587f824b927a5d"}}