{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2000:J6KO7GAN6YB24N7RZSYUZN3GSS","short_pith_number":"pith:J6KO7GAN","canonical_record":{"source":{"id":"gr-qc/0009069","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"2000-09-19T15:39:43Z","cross_cats_sorted":[],"title_canon_sha256":"865a9126e2da33f371ac09b80caaba54d11f4a659c22401ea6e5cf3b92472d7b","abstract_canon_sha256":"fcb9de0bc3dcbbb5d631e06fcae8c600cffb12b4acfca7e7bd01aedcdf4bd8b7"},"schema_version":"1.0"},"canonical_sha256":"4f94ef980df603ae37f1ccb14cb766949612573f0b53a0ffd861edd84cf22422","source":{"kind":"arxiv","id":"gr-qc/0009069","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"gr-qc/0009069","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/0009069v2","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/0009069","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"pith_short_12","alias_value":"J6KO7GAN6YB2","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"pith_short_16","alias_value":"J6KO7GAN6YB24N7R","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"pith_short_8","alias_value":"J6KO7GAN","created_at":"2026-07-04T16:19:41Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2000:J6KO7GAN6YB24N7RZSYUZN3GSS","target":"record","payload":{"canonical_record":{"source":{"id":"gr-qc/0009069","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"gr-qc","submitted_at":"2000-09-19T15:39:43Z","cross_cats_sorted":[],"title_canon_sha256":"865a9126e2da33f371ac09b80caaba54d11f4a659c22401ea6e5cf3b92472d7b","abstract_canon_sha256":"fcb9de0bc3dcbbb5d631e06fcae8c600cffb12b4acfca7e7bd01aedcdf4bd8b7"},"schema_version":"1.0"},"canonical_sha256":"4f94ef980df603ae37f1ccb14cb766949612573f0b53a0ffd861edd84cf22422","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:19:41.971923Z","signature_b64":"lHzwyXFqQ4asngx9FcXLtXNl4/59XPGHMDBF2+L7+T5OGIujfCeYPHk+V1kajJ8Oi4iixt4dypRVyyTKs99cCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4f94ef980df603ae37f1ccb14cb766949612573f0b53a0ffd861edd84cf22422","last_reissued_at":"2026-07-04T16:19:41.971569Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:19:41.971569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"gr-qc/0009069","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":"2026-07-04T16:19:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CFvWmjJS1wtfVUfh2aZRcptvL/l+VDqgKQhYFcyQWQyPf3IKqT4bkMMWk9P+LXmL2HJ/MNaI0qkXD4Jh/2iADw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T22:18:57.858835Z"},"content_sha256":"590b288aa8b27b2170351c36871b33e61355cb5c8a78d83d107c9fa45e27722c","schema_version":"1.0","event_id":"sha256:590b288aa8b27b2170351c36871b33e61355cb5c8a78d83d107c9fa45e27722c"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2000:J6KO7GAN6YB24N7RZSYUZN3GSS","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Conformal Black Hole Solutions of Axi-Dilaton Gravity in D-dimensions","license":"","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"H. Cebeci, T. Dereli (METU)","submitted_at":"2000-09-19T15:39:43Z","abstract_excerpt":"Static, spherically symmetric solutions of axi-dilaton gravity in $D$ dimensions is given in the Brans-Dicke frame for arbitrary values of the Brans-Dicke constant $\\omega$ and an axion-dilaton coupling parameter $k$. The mass and the dilaton and axion charges are determined and a BPS bound is derived. There exists a one parameter family of black hole solutions in the scale invariant limit."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/0009069","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/gr-qc/0009069/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":"2026-07-04T16:19:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Fn/3euG9+yEoD3Hk2RXVuqslkfo9Gbh5dfS45WFEeHHVwCxH5/F/jLWXmUFWdLtxO5gu6eRZpWZNMpmtwEOWAg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-07-04T22:18:57.859233Z"},"content_sha256":"3cf3b5d96ac42af83c26de4f476690ede09c9f4151b22787853e1c2ad6c36f93","schema_version":"1.0","event_id":"sha256:3cf3b5d96ac42af83c26de4f476690ede09c9f4151b22787853e1c2ad6c36f93"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/J6KO7GAN6YB24N7RZSYUZN3GSS/bundle.json","state_url":"https://pith.science/pith/J6KO7GAN6YB24N7RZSYUZN3GSS/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/J6KO7GAN6YB24N7RZSYUZN3GSS/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":"2026-07-04T22:18:57Z","links":{"resolver":"https://pith.science/pith/J6KO7GAN6YB24N7RZSYUZN3GSS","bundle":"https://pith.science/pith/J6KO7GAN6YB24N7RZSYUZN3GSS/bundle.json","state":"https://pith.science/pith/J6KO7GAN6YB24N7RZSYUZN3GSS/state.json","well_known_bundle":"https://pith.science/.well-known/pith/J6KO7GAN6YB24N7RZSYUZN3GSS/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2000:J6KO7GAN6YB24N7RZSYUZN3GSS","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":"fcb9de0bc3dcbbb5d631e06fcae8c600cffb12b4acfca7e7bd01aedcdf4bd8b7","cross_cats_sorted":[],"license":"","primary_cat":"gr-qc","submitted_at":"2000-09-19T15:39:43Z","title_canon_sha256":"865a9126e2da33f371ac09b80caaba54d11f4a659c22401ea6e5cf3b92472d7b"},"schema_version":"1.0","source":{"id":"gr-qc/0009069","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"gr-qc/0009069","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"arxiv_version","alias_value":"gr-qc/0009069v2","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.gr-qc/0009069","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"pith_short_12","alias_value":"J6KO7GAN6YB2","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"pith_short_16","alias_value":"J6KO7GAN6YB24N7R","created_at":"2026-07-04T16:19:41Z"},{"alias_kind":"pith_short_8","alias_value":"J6KO7GAN","created_at":"2026-07-04T16:19:41Z"}],"graph_snapshots":[{"event_id":"sha256:3cf3b5d96ac42af83c26de4f476690ede09c9f4151b22787853e1c2ad6c36f93","target":"graph","created_at":"2026-07-04T16:19:41Z","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/gr-qc/0009069/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Static, spherically symmetric solutions of axi-dilaton gravity in $D$ dimensions is given in the Brans-Dicke frame for arbitrary values of the Brans-Dicke constant $\\omega$ and an axion-dilaton coupling parameter $k$. The mass and the dilaton and axion charges are determined and a BPS bound is derived. There exists a one parameter family of black hole solutions in the scale invariant limit.","authors_text":"H. Cebeci, T. Dereli (METU)","cross_cats":[],"headline":"","license":"","primary_cat":"gr-qc","submitted_at":"2000-09-19T15:39:43Z","title":"Conformal Black Hole Solutions of Axi-Dilaton Gravity in D-dimensions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"gr-qc/0009069","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":"sha256:590b288aa8b27b2170351c36871b33e61355cb5c8a78d83d107c9fa45e27722c","target":"record","created_at":"2026-07-04T16:19:41Z","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":"fcb9de0bc3dcbbb5d631e06fcae8c600cffb12b4acfca7e7bd01aedcdf4bd8b7","cross_cats_sorted":[],"license":"","primary_cat":"gr-qc","submitted_at":"2000-09-19T15:39:43Z","title_canon_sha256":"865a9126e2da33f371ac09b80caaba54d11f4a659c22401ea6e5cf3b92472d7b"},"schema_version":"1.0","source":{"id":"gr-qc/0009069","kind":"arxiv","version":2}},"canonical_sha256":"4f94ef980df603ae37f1ccb14cb766949612573f0b53a0ffd861edd84cf22422","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"4f94ef980df603ae37f1ccb14cb766949612573f0b53a0ffd861edd84cf22422","first_computed_at":"2026-07-04T16:19:41.971569Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T16:19:41.971569Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"lHzwyXFqQ4asngx9FcXLtXNl4/59XPGHMDBF2+L7+T5OGIujfCeYPHk+V1kajJ8Oi4iixt4dypRVyyTKs99cCw==","signature_status":"signed_v1","signed_at":"2026-07-04T16:19:41.971923Z","signed_message":"canonical_sha256_bytes"},"source_id":"gr-qc/0009069","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:590b288aa8b27b2170351c36871b33e61355cb5c8a78d83d107c9fa45e27722c","sha256:3cf3b5d96ac42af83c26de4f476690ede09c9f4151b22787853e1c2ad6c36f93"],"state_sha256":"c6ba07806e704803da903ecc3da72198f7c69dec961aedcc2116eeb63e2cca32"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"3LUxSinrLNYzHcjn3+022msMDBkXXNZeVjUVsROXruP8Rs7H0+a7ju8UE65yV0wqd/MdExGKBbQ+00cY95swDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-07-04T22:18:57.861775Z","bundle_sha256":"bfa3aa873928870bfcd7eb0b89bef7a5d316e2267012697eb8a4a797d3ddb182"}}