{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2009:SEJATHUJCFECAE2CHDQEZUCHRI","short_pith_number":"pith:SEJATHUJ","canonical_record":{"source":{"id":"0904.1777","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-04-11T04:22:23Z","cross_cats_sorted":[],"title_canon_sha256":"fc443d7dd97e39ffd508c349b212419a0b7ec0cc554827e16f64d0ad4d255424","abstract_canon_sha256":"0acea590bf26b5ea56d8138540b0383e00a38f05b9dee855df562d99af55d4c6"},"schema_version":"1.0"},"canonical_sha256":"9112099e89114820134238e04cd0478a08d8353c131a1219059e968f36f08745","source":{"kind":"arxiv","id":"0904.1777","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0904.1777","created_at":"2026-05-18T02:14:06Z"},{"alias_kind":"arxiv_version","alias_value":"0904.1777v2","created_at":"2026-05-18T02:14:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.1777","created_at":"2026-05-18T02:14:06Z"},{"alias_kind":"pith_short_12","alias_value":"SEJATHUJCFEC","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_16","alias_value":"SEJATHUJCFECAE2C","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_8","alias_value":"SEJATHUJ","created_at":"2026-05-18T12:26:01Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2009:SEJATHUJCFECAE2CHDQEZUCHRI","target":"record","payload":{"canonical_record":{"source":{"id":"0904.1777","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-04-11T04:22:23Z","cross_cats_sorted":[],"title_canon_sha256":"fc443d7dd97e39ffd508c349b212419a0b7ec0cc554827e16f64d0ad4d255424","abstract_canon_sha256":"0acea590bf26b5ea56d8138540b0383e00a38f05b9dee855df562d99af55d4c6"},"schema_version":"1.0"},"canonical_sha256":"9112099e89114820134238e04cd0478a08d8353c131a1219059e968f36f08745","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:14:06.451444Z","signature_b64":"1DeVrs4LctxuwXCQvh/kbHSGFbWKb9Y2V+idRcUqT7szVGAZBvkSdKT5PTNJrucjeAMMUZ/j9xaFm0veiHciDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9112099e89114820134238e04cd0478a08d8353c131a1219059e968f36f08745","last_reissued_at":"2026-05-18T02:14:06.450820Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:14:06.450820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"0904.1777","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":"2026-05-18T02:14:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fX6G6RrLZKZBWCm6vVH3b1pITquAaebvB5utdZ3MypiUiw/UeOv4e7riU8nm2ZS1jZ4v+464pvKMuyGBwGQsDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T19:25:01.320533Z"},"content_sha256":"789ccf4cedfe4f3cc7efde27c7f13d60de68bbce6ccd978d23093d811f9a6c0c","schema_version":"1.0","event_id":"sha256:789ccf4cedfe4f3cc7efde27c7f13d60de68bbce6ccd978d23093d811f9a6c0c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2009:SEJATHUJCFECAE2CHDQEZUCHRI","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Thermodynamics of Charged Brans-Dicke AdS Black Holes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"A. Sheykhi, M. M. Yazdanpanah","submitted_at":"2009-04-11T04:22:23Z","abstract_excerpt":"It is well-known that in four dimensions, black hole solution of the Brans-Dikce-Maxwell equations is just the Reissner-Nordstrom solution with a constant scalar field. However, in $n\\geq4$ dimensions, the solution is not yet the $(n+1)$-dimensional Reissner-Nordstrom solution and the scalar field is not a constant in general. In this paper, by applying a conformal transformation to the dilaton gravity theory, we derive a class of black hole solutions in $(n+1)$-dimensional $(n\\geq 4)$ Brans-Dikce-Maxwell theory in the background of anti-de Sitter universe. We obtain the conserved and thermody"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.1777","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":"2026-05-18T02:14:06Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"yMP9CS4YMWGBkuM2gyAVxci2KK23Jfdqr7b0uGaSFKTk7ijkqPoi/7hACqFbABF07RFTD9vHgqjy1SOLkcpiBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T19:25:01.321309Z"},"content_sha256":"b15892ac08ebf2bdb572427f2e4ac2a476f9b284311597fb09639b4db6faa869","schema_version":"1.0","event_id":"sha256:b15892ac08ebf2bdb572427f2e4ac2a476f9b284311597fb09639b4db6faa869"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/SEJATHUJCFECAE2CHDQEZUCHRI/bundle.json","state_url":"https://pith.science/pith/SEJATHUJCFECAE2CHDQEZUCHRI/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/SEJATHUJCFECAE2CHDQEZUCHRI/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":"2026-06-08T19:25:01Z","links":{"resolver":"https://pith.science/pith/SEJATHUJCFECAE2CHDQEZUCHRI","bundle":"https://pith.science/pith/SEJATHUJCFECAE2CHDQEZUCHRI/bundle.json","state":"https://pith.science/pith/SEJATHUJCFECAE2CHDQEZUCHRI/state.json","well_known_bundle":"https://pith.science/.well-known/pith/SEJATHUJCFECAE2CHDQEZUCHRI/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2009:SEJATHUJCFECAE2CHDQEZUCHRI","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":"0acea590bf26b5ea56d8138540b0383e00a38f05b9dee855df562d99af55d4c6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-04-11T04:22:23Z","title_canon_sha256":"fc443d7dd97e39ffd508c349b212419a0b7ec0cc554827e16f64d0ad4d255424"},"schema_version":"1.0","source":{"id":"0904.1777","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"0904.1777","created_at":"2026-05-18T02:14:06Z"},{"alias_kind":"arxiv_version","alias_value":"0904.1777v2","created_at":"2026-05-18T02:14:06Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0904.1777","created_at":"2026-05-18T02:14:06Z"},{"alias_kind":"pith_short_12","alias_value":"SEJATHUJCFEC","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_16","alias_value":"SEJATHUJCFECAE2C","created_at":"2026-05-18T12:26:01Z"},{"alias_kind":"pith_short_8","alias_value":"SEJATHUJ","created_at":"2026-05-18T12:26:01Z"}],"graph_snapshots":[{"event_id":"sha256:b15892ac08ebf2bdb572427f2e4ac2a476f9b284311597fb09639b4db6faa869","target":"graph","created_at":"2026-05-18T02:14:06Z","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":"It is well-known that in four dimensions, black hole solution of the Brans-Dikce-Maxwell equations is just the Reissner-Nordstrom solution with a constant scalar field. However, in $n\\geq4$ dimensions, the solution is not yet the $(n+1)$-dimensional Reissner-Nordstrom solution and the scalar field is not a constant in general. In this paper, by applying a conformal transformation to the dilaton gravity theory, we derive a class of black hole solutions in $(n+1)$-dimensional $(n\\geq 4)$ Brans-Dikce-Maxwell theory in the background of anti-de Sitter universe. We obtain the conserved and thermody","authors_text":"A. Sheykhi, M. M. Yazdanpanah","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-04-11T04:22:23Z","title":"Thermodynamics of Charged Brans-Dicke AdS Black Holes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0904.1777","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":"sha256:789ccf4cedfe4f3cc7efde27c7f13d60de68bbce6ccd978d23093d811f9a6c0c","target":"record","created_at":"2026-05-18T02:14:06Z","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":"0acea590bf26b5ea56d8138540b0383e00a38f05b9dee855df562d99af55d4c6","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2009-04-11T04:22:23Z","title_canon_sha256":"fc443d7dd97e39ffd508c349b212419a0b7ec0cc554827e16f64d0ad4d255424"},"schema_version":"1.0","source":{"id":"0904.1777","kind":"arxiv","version":2}},"canonical_sha256":"9112099e89114820134238e04cd0478a08d8353c131a1219059e968f36f08745","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9112099e89114820134238e04cd0478a08d8353c131a1219059e968f36f08745","first_computed_at":"2026-05-18T02:14:06.450820Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:14:06.450820Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"1DeVrs4LctxuwXCQvh/kbHSGFbWKb9Y2V+idRcUqT7szVGAZBvkSdKT5PTNJrucjeAMMUZ/j9xaFm0veiHciDg==","signature_status":"signed_v1","signed_at":"2026-05-18T02:14:06.451444Z","signed_message":"canonical_sha256_bytes"},"source_id":"0904.1777","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:789ccf4cedfe4f3cc7efde27c7f13d60de68bbce6ccd978d23093d811f9a6c0c","sha256:b15892ac08ebf2bdb572427f2e4ac2a476f9b284311597fb09639b4db6faa869"],"state_sha256":"d00139e04a2bd9c789fb25cead8e7e336ea30df2023efa6360a85b3c092a2f3f"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"OZAG8voEfvnOFj833lXuD4UKG9wGfLXe5IU0VkkkQfTW2ZWwv4WPMolIZ6WImJkvzMoAUO3SVNjuWfQf7zIhAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T19:25:01.326118Z","bundle_sha256":"f775e3f2ebc0ea05a42c2c3e982f5cde27bf2eb49e841ff72eeca9850c679e5f"}}