{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2018:DDX5LFCKOEDXQQYP5QBMQZ3FVO","short_pith_number":"pith:DDX5LFCK","canonical_record":{"source":{"id":"1805.12593","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-05-29T14:20:58Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"45e81e51c581864e96638b4bc0892afc45f4ede525ecb9b94bbd04aa1bbf5d58","abstract_canon_sha256":"e59bae69ba839ab6f0e50a839817bd13f02615c3db53de08f912f69f7a3ffe43"},"schema_version":"1.0"},"canonical_sha256":"18efd5944a710778430fec02c86765abae53b85ed8ac9ad9c2b6104530a9ca33","source":{"kind":"arxiv","id":"1805.12593","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.12593","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"arxiv_version","alias_value":"1805.12593v2","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.12593","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"pith_short_12","alias_value":"DDX5LFCKOEDX","created_at":"2026-05-18T12:32:19Z"},{"alias_kind":"pith_short_16","alias_value":"DDX5LFCKOEDXQQYP","created_at":"2026-05-18T12:32:19Z"},{"alias_kind":"pith_short_8","alias_value":"DDX5LFCK","created_at":"2026-05-18T12:32:19Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2018:DDX5LFCKOEDXQQYP5QBMQZ3FVO","target":"record","payload":{"canonical_record":{"source":{"id":"1805.12593","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-05-29T14:20:58Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"45e81e51c581864e96638b4bc0892afc45f4ede525ecb9b94bbd04aa1bbf5d58","abstract_canon_sha256":"e59bae69ba839ab6f0e50a839817bd13f02615c3db53de08f912f69f7a3ffe43"},"schema_version":"1.0"},"canonical_sha256":"18efd5944a710778430fec02c86765abae53b85ed8ac9ad9c2b6104530a9ca33","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:05:45.426409Z","signature_b64":"yfeqDxFYA4DagZg/Eo55WlSLdCGNuuaiYKnLKE8z5lQqWIKpSDiRXlvoKHbbJ5lwfVeHVECz2mP/DEgBvZKmBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"18efd5944a710778430fec02c86765abae53b85ed8ac9ad9c2b6104530a9ca33","last_reissued_at":"2026-05-18T00:05:45.425748Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:05:45.425748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1805.12593","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":"2026-05-18T00:05:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5uJUYNIUpjosOMndDp7bG1M+qfjSy+4ktoC8hXciYwArdK+/McvjH4ID8jm2edGA9xFNgHmBDqBTq3IxI0VQCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T08:15:36.208573Z"},"content_sha256":"7a5be2d92460e8d3edb025727312b81f2d0d97e640cb7c91b3b376092388f3eb","schema_version":"1.0","event_id":"sha256:7a5be2d92460e8d3edb025727312b81f2d0d97e640cb7c91b3b376092388f3eb"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2018:DDX5LFCKOEDXQQYP5QBMQZ3FVO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Spherically symmetric charged black hole in conformal teleparallel equivalent of general relativity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"gr-qc","authors_text":"G.G.L. Nashed, Kazuharu Bamba","submitted_at":"2018-05-29T14:20:58Z","abstract_excerpt":"We study 4-dimensional non-charged and charged spherically symmetric spacetimes in conformal teleparallel equivalent of general relativity. We apply the gravitational field equations in non-charged and charged spacetimes to the diagonal and non-diagonal vierbeins and derive their sets of the non-linear differential equations. It is demonstrated that the Schwarzschild, for the non-charged case, and the Reissner-Nordstr\\\"om, for the charged case, are the only black hole solutions for the spherically symmetric case in the framework of the conformal teleparallel equivalent of general relativity th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.12593","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":"2026-05-18T00:05:45Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YO0xVWHishyUlXVvNdgLuvMlkrSP7GJzpEDJ3YHzQ44hGh8GrYBCUbYEFbMc5IAlNsWvVqXKQ3nXCOAtB5bhCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-28T08:15:36.208918Z"},"content_sha256":"bda1ad3b1dded6e268a0ad31e2b56361af5861177af724568aa48c6d916ac430","schema_version":"1.0","event_id":"sha256:bda1ad3b1dded6e268a0ad31e2b56361af5861177af724568aa48c6d916ac430"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/DDX5LFCKOEDXQQYP5QBMQZ3FVO/bundle.json","state_url":"https://pith.science/pith/DDX5LFCKOEDXQQYP5QBMQZ3FVO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/DDX5LFCKOEDXQQYP5QBMQZ3FVO/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":"2026-05-28T08:15:36Z","links":{"resolver":"https://pith.science/pith/DDX5LFCKOEDXQQYP5QBMQZ3FVO","bundle":"https://pith.science/pith/DDX5LFCKOEDXQQYP5QBMQZ3FVO/bundle.json","state":"https://pith.science/pith/DDX5LFCKOEDXQQYP5QBMQZ3FVO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/DDX5LFCKOEDXQQYP5QBMQZ3FVO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2018:DDX5LFCKOEDXQQYP5QBMQZ3FVO","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":"e59bae69ba839ab6f0e50a839817bd13f02615c3db53de08f912f69f7a3ffe43","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-05-29T14:20:58Z","title_canon_sha256":"45e81e51c581864e96638b4bc0892afc45f4ede525ecb9b94bbd04aa1bbf5d58"},"schema_version":"1.0","source":{"id":"1805.12593","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1805.12593","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"arxiv_version","alias_value":"1805.12593v2","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1805.12593","created_at":"2026-05-18T00:05:45Z"},{"alias_kind":"pith_short_12","alias_value":"DDX5LFCKOEDX","created_at":"2026-05-18T12:32:19Z"},{"alias_kind":"pith_short_16","alias_value":"DDX5LFCKOEDXQQYP","created_at":"2026-05-18T12:32:19Z"},{"alias_kind":"pith_short_8","alias_value":"DDX5LFCK","created_at":"2026-05-18T12:32:19Z"}],"graph_snapshots":[{"event_id":"sha256:bda1ad3b1dded6e268a0ad31e2b56361af5861177af724568aa48c6d916ac430","target":"graph","created_at":"2026-05-18T00:05:45Z","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 study 4-dimensional non-charged and charged spherically symmetric spacetimes in conformal teleparallel equivalent of general relativity. We apply the gravitational field equations in non-charged and charged spacetimes to the diagonal and non-diagonal vierbeins and derive their sets of the non-linear differential equations. It is demonstrated that the Schwarzschild, for the non-charged case, and the Reissner-Nordstr\\\"om, for the charged case, are the only black hole solutions for the spherically symmetric case in the framework of the conformal teleparallel equivalent of general relativity th","authors_text":"G.G.L. Nashed, Kazuharu Bamba","cross_cats":["hep-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-05-29T14:20:58Z","title":"Spherically symmetric charged black hole in conformal teleparallel equivalent of general relativity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1805.12593","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":"sha256:7a5be2d92460e8d3edb025727312b81f2d0d97e640cb7c91b3b376092388f3eb","target":"record","created_at":"2026-05-18T00:05:45Z","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":"e59bae69ba839ab6f0e50a839817bd13f02615c3db53de08f912f69f7a3ffe43","cross_cats_sorted":["hep-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2018-05-29T14:20:58Z","title_canon_sha256":"45e81e51c581864e96638b4bc0892afc45f4ede525ecb9b94bbd04aa1bbf5d58"},"schema_version":"1.0","source":{"id":"1805.12593","kind":"arxiv","version":2}},"canonical_sha256":"18efd5944a710778430fec02c86765abae53b85ed8ac9ad9c2b6104530a9ca33","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"18efd5944a710778430fec02c86765abae53b85ed8ac9ad9c2b6104530a9ca33","first_computed_at":"2026-05-18T00:05:45.425748Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:05:45.425748Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"yfeqDxFYA4DagZg/Eo55WlSLdCGNuuaiYKnLKE8z5lQqWIKpSDiRXlvoKHbbJ5lwfVeHVECz2mP/DEgBvZKmBg==","signature_status":"signed_v1","signed_at":"2026-05-18T00:05:45.426409Z","signed_message":"canonical_sha256_bytes"},"source_id":"1805.12593","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7a5be2d92460e8d3edb025727312b81f2d0d97e640cb7c91b3b376092388f3eb","sha256:bda1ad3b1dded6e268a0ad31e2b56361af5861177af724568aa48c6d916ac430"],"state_sha256":"8d75761388899e30791c5159636b052467dd1d4f9e0fe79b864555a35474d75e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"UBNp085r48nvS49WTZ6kmcaV+SPeiY7ipRjQ1la9K8ZvdUFe7QQh1Caz3pvdI8mI1cgxvde7YRzEOEvkSYzlAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-28T08:15:36.211556Z","bundle_sha256":"aff60bf6655248f8e76a5e91bf7c8a54018a5d4fa1c5dd76cfc5aa81a7888bc6"}}