{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2021:BFVRHZ3SRNTNROORWXLMRDKYFA","short_pith_number":"pith:BFVRHZ3S","canonical_record":{"source":{"id":"2102.10541","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-21T07:56:52Z","cross_cats_sorted":[],"title_canon_sha256":"efd696153c1059bb194cb93bd9b1771484898f7e63bd242e0108032c07b0a885","abstract_canon_sha256":"a9190582c9cef2ecaafebc6cec46b4d2e8a65db51607eaf230b27810c6e7a045"},"schema_version":"1.0"},"canonical_sha256":"096b13e7728b66d8b9d1b5d6c88d58280c74e5a7ac515a681a29ac24cd2ac28e","source":{"kind":"arxiv","id":"2102.10541","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2102.10541","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"arxiv_version","alias_value":"2102.10541v2","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.10541","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"pith_short_12","alias_value":"BFVRHZ3SRNTN","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"pith_short_16","alias_value":"BFVRHZ3SRNTNROOR","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"pith_short_8","alias_value":"BFVRHZ3S","created_at":"2026-07-05T03:02:46Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2021:BFVRHZ3SRNTNROORWXLMRDKYFA","target":"record","payload":{"canonical_record":{"source":{"id":"2102.10541","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-21T07:56:52Z","cross_cats_sorted":[],"title_canon_sha256":"efd696153c1059bb194cb93bd9b1771484898f7e63bd242e0108032c07b0a885","abstract_canon_sha256":"a9190582c9cef2ecaafebc6cec46b4d2e8a65db51607eaf230b27810c6e7a045"},"schema_version":"1.0"},"canonical_sha256":"096b13e7728b66d8b9d1b5d6c88d58280c74e5a7ac515a681a29ac24cd2ac28e","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T03:02:46.299792Z","signature_b64":"aQ+LfGnOFtBh1Qys7OZYXCerBN0N/5l99N/T5VlSGDNqELNAVnTaup4+OFadven+Ucbf4qcVydVrAlmMgzbtCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"096b13e7728b66d8b9d1b5d6c88d58280c74e5a7ac515a681a29ac24cd2ac28e","last_reissued_at":"2026-07-05T03:02:46.299279Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T03:02:46.299279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2102.10541","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":"2026-07-05T03:02:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Huzd6OIS2IoEoOhrDuvnbQNwXHt8YzTBRzXbHvILutFBme+5oWgnmCxvb/GQJC9h4iROB+7Di3/uhsTbGrNvCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T11:08:20.242566Z"},"content_sha256":"203a14bd8f1f19e0b8401695223bcb108e6795a00f9f21f6f1851ae4804c3ef4","schema_version":"1.0","event_id":"sha256:203a14bd8f1f19e0b8401695223bcb108e6795a00f9f21f6f1851ae4804c3ef4"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2021:BFVRHZ3SRNTNROORWXLMRDKYFA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Charged black hole and radiating solutions in entangled relativity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Edison Santos, Olivier Minazzoli","submitted_at":"2021-02-21T07:56:52Z","abstract_excerpt":"In this manuscript, we show that the external Schwarzschild metric can be a good approximation of exact black hole solutions of entangled relativity. Since entangled relativity cannot be defined from vacuum, the demonstrations need to rely on the definition of matter fields. The electromagnetic field being the easiest (and perhaps the only) existing matter field with infinite range to consider, we study the case of a charged black hole -- for which the solution of entangled relativity and a dilaton theory agree -- as well as the case of a pure radiation -- for which the solution of entangled r"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.10541","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/2102.10541/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":"2026-07-05T03:02:46Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"Mh6+3QISEyktUFh2pGeaD8HG84tDvr7o3gcl/3ZHuUP43WqSQr8B1AzfWp2p/Xd6bPBTmojC7iJkscu4/oH0BA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-04T11:08:20.243085Z"},"content_sha256":"05862873fb6707f7ecfabe081844d79b7752d36341f019a56835a473d46824e0","schema_version":"1.0","event_id":"sha256:05862873fb6707f7ecfabe081844d79b7752d36341f019a56835a473d46824e0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/BFVRHZ3SRNTNROORWXLMRDKYFA/bundle.json","state_url":"https://pith.science/pith/BFVRHZ3SRNTNROORWXLMRDKYFA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/BFVRHZ3SRNTNROORWXLMRDKYFA/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":"2026-08-04T11:08:20Z","links":{"resolver":"https://pith.science/pith/BFVRHZ3SRNTNROORWXLMRDKYFA","bundle":"https://pith.science/pith/BFVRHZ3SRNTNROORWXLMRDKYFA/bundle.json","state":"https://pith.science/pith/BFVRHZ3SRNTNROORWXLMRDKYFA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/BFVRHZ3SRNTNROORWXLMRDKYFA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:BFVRHZ3SRNTNROORWXLMRDKYFA","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":"a9190582c9cef2ecaafebc6cec46b4d2e8a65db51607eaf230b27810c6e7a045","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-21T07:56:52Z","title_canon_sha256":"efd696153c1059bb194cb93bd9b1771484898f7e63bd242e0108032c07b0a885"},"schema_version":"1.0","source":{"id":"2102.10541","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2102.10541","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"arxiv_version","alias_value":"2102.10541v2","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2102.10541","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"pith_short_12","alias_value":"BFVRHZ3SRNTN","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"pith_short_16","alias_value":"BFVRHZ3SRNTNROOR","created_at":"2026-07-05T03:02:46Z"},{"alias_kind":"pith_short_8","alias_value":"BFVRHZ3S","created_at":"2026-07-05T03:02:46Z"}],"graph_snapshots":[{"event_id":"sha256:05862873fb6707f7ecfabe081844d79b7752d36341f019a56835a473d46824e0","target":"graph","created_at":"2026-07-05T03:02:46Z","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/2102.10541/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this manuscript, we show that the external Schwarzschild metric can be a good approximation of exact black hole solutions of entangled relativity. Since entangled relativity cannot be defined from vacuum, the demonstrations need to rely on the definition of matter fields. The electromagnetic field being the easiest (and perhaps the only) existing matter field with infinite range to consider, we study the case of a charged black hole -- for which the solution of entangled relativity and a dilaton theory agree -- as well as the case of a pure radiation -- for which the solution of entangled r","authors_text":"Edison Santos, Olivier Minazzoli","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-21T07:56:52Z","title":"Charged black hole and radiating solutions in entangled relativity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2102.10541","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":"sha256:203a14bd8f1f19e0b8401695223bcb108e6795a00f9f21f6f1851ae4804c3ef4","target":"record","created_at":"2026-07-05T03:02:46Z","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":"a9190582c9cef2ecaafebc6cec46b4d2e8a65db51607eaf230b27810c6e7a045","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2021-02-21T07:56:52Z","title_canon_sha256":"efd696153c1059bb194cb93bd9b1771484898f7e63bd242e0108032c07b0a885"},"schema_version":"1.0","source":{"id":"2102.10541","kind":"arxiv","version":2}},"canonical_sha256":"096b13e7728b66d8b9d1b5d6c88d58280c74e5a7ac515a681a29ac24cd2ac28e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"096b13e7728b66d8b9d1b5d6c88d58280c74e5a7ac515a681a29ac24cd2ac28e","first_computed_at":"2026-07-05T03:02:46.299279Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T03:02:46.299279Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"aQ+LfGnOFtBh1Qys7OZYXCerBN0N/5l99N/T5VlSGDNqELNAVnTaup4+OFadven+Ucbf4qcVydVrAlmMgzbtCw==","signature_status":"signed_v1","signed_at":"2026-07-05T03:02:46.299792Z","signed_message":"canonical_sha256_bytes"},"source_id":"2102.10541","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:203a14bd8f1f19e0b8401695223bcb108e6795a00f9f21f6f1851ae4804c3ef4","sha256:05862873fb6707f7ecfabe081844d79b7752d36341f019a56835a473d46824e0"],"state_sha256":"0f91da25d5ac329d89d3895d1b13046cd555508074b30f14cba634569db865b4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"6poSngEHp2xVgEt9LvjYDnPVmlqyrNQFQ92Rw5GJrpUWkSH61AQrsizniTOahaLytcF6sj972IeBm+k6xbhABw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-04T11:08:20.248966Z","bundle_sha256":"75ad6fa379e815844e7dc6f755ff390c97e500794e10e7f0d2e4bd3570c08a85"}}