{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2002:RU6SPYL2SOAPRW3QCOIRVKD3LY","short_pith_number":"pith:RU6SPYL2","canonical_record":{"source":{"id":"hep-th/0201127","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-16T20:45:47Z","cross_cats_sorted":["astro-ph","gr-qc"],"title_canon_sha256":"f24017a8fe25f265f495c0260a5153eaf774d59fd9c51d4acb730e16a9002615","abstract_canon_sha256":"cd50bb004e94265de9b8d5f1d3f86fc2af75d14ff091cd5c616f6ebddb885e54"},"schema_version":"1.0"},"canonical_sha256":"8d3d27e17a9380f8db7013911aa87b5e2e348fa704896a3dcb6614654dababd2","source":{"kind":"arxiv","id":"hep-th/0201127","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0201127","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201127v1","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201127","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_12","alias_value":"RU6SPYL2SOAP","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_16","alias_value":"RU6SPYL2SOAPRW3Q","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_8","alias_value":"RU6SPYL2","created_at":"2026-07-04T16:34:31Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2002:RU6SPYL2SOAPRW3QCOIRVKD3LY","target":"record","payload":{"canonical_record":{"source":{"id":"hep-th/0201127","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2002-01-16T20:45:47Z","cross_cats_sorted":["astro-ph","gr-qc"],"title_canon_sha256":"f24017a8fe25f265f495c0260a5153eaf774d59fd9c51d4acb730e16a9002615","abstract_canon_sha256":"cd50bb004e94265de9b8d5f1d3f86fc2af75d14ff091cd5c616f6ebddb885e54"},"schema_version":"1.0"},"canonical_sha256":"8d3d27e17a9380f8db7013911aa87b5e2e348fa704896a3dcb6614654dababd2","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:34:31.953877Z","signature_b64":"Ars142faBMjKX4jKMFu7DzLA5Ip8nkA2v7AD/zsvHpwFswXLLzl6v2M38kCo5dgr3LlunfWLbF/jlHcr/eShCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"8d3d27e17a9380f8db7013911aa87b5e2e348fa704896a3dcb6614654dababd2","last_reissued_at":"2026-07-04T16:34:31.953530Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:34:31.953530Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"hep-th/0201127","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-07-04T16:34:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"znDpYwa8+e0ma6pSy5lZ1fqG6hCkIhZTYPHZ8W4kTaxvvWn6h/O/8GlU5t6cCaSoaseHWXRm3TW2kJf+qV3SDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T22:08:23.219312Z"},"content_sha256":"d92b06203b592a821223a498f65baa56c579bbd5caaeebd72589866edf457176","schema_version":"1.0","event_id":"sha256:d92b06203b592a821223a498f65baa56c579bbd5caaeebd72589866edf457176"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2002:RU6SPYL2SOAPRW3QCOIRVKD3LY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Strong Brane Gravity and the Radion at Low Energies","license":"","headline":"","cross_cats":["astro-ph","gr-qc"],"primary_cat":"hep-th","authors_text":"T. Wiseman","submitted_at":"2002-01-16T20:45:47Z","abstract_excerpt":"For the 2-brane Randall-Sundrum model, we calculate the bulk geometry for strong gravity, in the low matter density regime, for slowly varying matter sources. This is relevant for astrophysical or cosmological applications. The warped compactification means the radion can not be written as a homogeneous mode in the orbifold coordinate, and we introduce it by extending the coordinate patch approach of the linear theory to the non-linear case. The negative tension brane is taken to be in vacuum. For conformally invariant matter on the positive tension brane, we solve the bulk geometry as a deriv"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201127","kind":"arxiv","version":1},"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-th/0201127/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":"2026-07-04T16:34:31Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xS9Oz7IrK3gRIHbt09kkKRrRPQW2JeLvO4UHcrGv+VHO9voN+Isf1k8fyrhhEXWlCu6vY0oHfSwT3vAnCyexDQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T22:08:23.219703Z"},"content_sha256":"1980326e421d6a6f8c756a2f4d09ac83da9489caa93b99d5598f1d270ab829c5","schema_version":"1.0","event_id":"sha256:1980326e421d6a6f8c756a2f4d09ac83da9489caa93b99d5598f1d270ab829c5"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/RU6SPYL2SOAPRW3QCOIRVKD3LY/bundle.json","state_url":"https://pith.science/pith/RU6SPYL2SOAPRW3QCOIRVKD3LY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/RU6SPYL2SOAPRW3QCOIRVKD3LY/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":"2026-07-04T22:08:23Z","links":{"resolver":"https://pith.science/pith/RU6SPYL2SOAPRW3QCOIRVKD3LY","bundle":"https://pith.science/pith/RU6SPYL2SOAPRW3QCOIRVKD3LY/bundle.json","state":"https://pith.science/pith/RU6SPYL2SOAPRW3QCOIRVKD3LY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/RU6SPYL2SOAPRW3QCOIRVKD3LY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2002:RU6SPYL2SOAPRW3QCOIRVKD3LY","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":"cd50bb004e94265de9b8d5f1d3f86fc2af75d14ff091cd5c616f6ebddb885e54","cross_cats_sorted":["astro-ph","gr-qc"],"license":"","primary_cat":"hep-th","submitted_at":"2002-01-16T20:45:47Z","title_canon_sha256":"f24017a8fe25f265f495c0260a5153eaf774d59fd9c51d4acb730e16a9002615"},"schema_version":"1.0","source":{"id":"hep-th/0201127","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"hep-th/0201127","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0201127v1","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0201127","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_12","alias_value":"RU6SPYL2SOAP","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_16","alias_value":"RU6SPYL2SOAPRW3Q","created_at":"2026-07-04T16:34:31Z"},{"alias_kind":"pith_short_8","alias_value":"RU6SPYL2","created_at":"2026-07-04T16:34:31Z"}],"graph_snapshots":[{"event_id":"sha256:1980326e421d6a6f8c756a2f4d09ac83da9489caa93b99d5598f1d270ab829c5","target":"graph","created_at":"2026-07-04T16:34:31Z","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-th/0201127/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"For the 2-brane Randall-Sundrum model, we calculate the bulk geometry for strong gravity, in the low matter density regime, for slowly varying matter sources. This is relevant for astrophysical or cosmological applications. The warped compactification means the radion can not be written as a homogeneous mode in the orbifold coordinate, and we introduce it by extending the coordinate patch approach of the linear theory to the non-linear case. The negative tension brane is taken to be in vacuum. For conformally invariant matter on the positive tension brane, we solve the bulk geometry as a deriv","authors_text":"T. Wiseman","cross_cats":["astro-ph","gr-qc"],"headline":"","license":"","primary_cat":"hep-th","submitted_at":"2002-01-16T20:45:47Z","title":"Strong Brane Gravity and the Radion at Low Energies"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0201127","kind":"arxiv","version":1},"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:d92b06203b592a821223a498f65baa56c579bbd5caaeebd72589866edf457176","target":"record","created_at":"2026-07-04T16:34:31Z","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":"cd50bb004e94265de9b8d5f1d3f86fc2af75d14ff091cd5c616f6ebddb885e54","cross_cats_sorted":["astro-ph","gr-qc"],"license":"","primary_cat":"hep-th","submitted_at":"2002-01-16T20:45:47Z","title_canon_sha256":"f24017a8fe25f265f495c0260a5153eaf774d59fd9c51d4acb730e16a9002615"},"schema_version":"1.0","source":{"id":"hep-th/0201127","kind":"arxiv","version":1}},"canonical_sha256":"8d3d27e17a9380f8db7013911aa87b5e2e348fa704896a3dcb6614654dababd2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"8d3d27e17a9380f8db7013911aa87b5e2e348fa704896a3dcb6614654dababd2","first_computed_at":"2026-07-04T16:34:31.953530Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:34:31.953530Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"Ars142faBMjKX4jKMFu7DzLA5Ip8nkA2v7AD/zsvHpwFswXLLzl6v2M38kCo5dgr3LlunfWLbF/jlHcr/eShCQ==","signature_status":"signed_v1","signed_at":"2026-07-04T16:34:31.953877Z","signed_message":"canonical_sha256_bytes"},"source_id":"hep-th/0201127","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d92b06203b592a821223a498f65baa56c579bbd5caaeebd72589866edf457176","sha256:1980326e421d6a6f8c756a2f4d09ac83da9489caa93b99d5598f1d270ab829c5"],"state_sha256":"fad230e74db25de60faf96e5f9869adab9b36af751413dd247913bd404323a7d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YFfqe4tLKBwye4+VAR9sd5MP2xtsy8UTFORm5Q6aSQVGEY2+cpJrtBgkyEnIj6CIQlGpR4PJxUtTDp9v/0i+Cw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-04T22:08:23.221685Z","bundle_sha256":"6d5616937f240763df3234446a38ff1803fcfcdc8859fd02b3ded69655b81d57"}}