{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:WSRD6GF7EFMKSESOM24HSYEFAD","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":"9911d651fb272c1a621555ef2015119e32cf8ab49f896087417a7e3488b1946d","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-11-26T23:20:33Z","title_canon_sha256":"47cdaf92a2b951c33226944735361b9d48800cdff863088fbed1d7bbaf359a9a"},"schema_version":"1.0","source":{"id":"2411.17938","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2411.17938","created_at":"2026-07-05T09:41:09Z"},{"alias_kind":"arxiv_version","alias_value":"2411.17938v1","created_at":"2026-07-05T09:41:09Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.17938","created_at":"2026-07-05T09:41:09Z"},{"alias_kind":"pith_short_12","alias_value":"WSRD6GF7EFMK","created_at":"2026-07-05T09:41:09Z"},{"alias_kind":"pith_short_16","alias_value":"WSRD6GF7EFMKSESO","created_at":"2026-07-05T09:41:09Z"},{"alias_kind":"pith_short_8","alias_value":"WSRD6GF7","created_at":"2026-07-05T09:41:09Z"}],"graph_snapshots":[{"event_id":"sha256:c84474d5596443849734cc1512eaa3a4f3c15e88b6f9aa6030233be7bb823f32","target":"graph","created_at":"2026-07-05T09:41:09Z","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/2411.17938/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In this work we extend the proof of Ryan Unger and Christoph Kehle's work, \"Gravitational collapse to extremal black holes and the third law of black hole thermodynamics\", to construct examples of black hole formation from regular, one-ended asymptotically flat Cauchy data for the Einstein-Maxwell charged scalar field system in maximally-symmetric 3+1 dimensional spacetime which are exactly isometric to $dS_{4}/AdS_{4}$ Reissner N\\\"ordstrom black holes after a finite advanced time along the event horizon. Furthermore, the apparent horizon coincides with that of a vacuum at finite advanced time","authors_text":"Ryan Marin","cross_cats":["math-ph","math.MP"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-11-26T23:20:33Z","title":"$C^{k}$-regular extremal black holes in maximally-symmetric spacetime and the third law of black hole thermodynamics"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.17938","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":"sha256:1d67804e925d8605192c49e20e3f6a2ea5fc78b39cb546af01da774972207b64","target":"record","created_at":"2026-07-05T09:41:09Z","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":"9911d651fb272c1a621555ef2015119e32cf8ab49f896087417a7e3488b1946d","cross_cats_sorted":["math-ph","math.MP"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2024-11-26T23:20:33Z","title_canon_sha256":"47cdaf92a2b951c33226944735361b9d48800cdff863088fbed1d7bbaf359a9a"},"schema_version":"1.0","source":{"id":"2411.17938","kind":"arxiv","version":1}},"canonical_sha256":"b4a23f18bf2158a9124e66b879608500fa213722fa225e5e7f6d202765a3424e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b4a23f18bf2158a9124e66b879608500fa213722fa225e5e7f6d202765a3424e","first_computed_at":"2026-07-05T09:41:09.216512Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T09:41:09.216512Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"llcz+4T+bf9NaC7ZWvwMJyKDUpPRBJhQuV/hp9nkt7DVRDkDklOvsteNX2DW57pCQC+nbebzol/BkpC+qoG9CA==","signature_status":"signed_v1","signed_at":"2026-07-05T09:41:09.216959Z","signed_message":"canonical_sha256_bytes"},"source_id":"2411.17938","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:1d67804e925d8605192c49e20e3f6a2ea5fc78b39cb546af01da774972207b64","sha256:c84474d5596443849734cc1512eaa3a4f3c15e88b6f9aa6030233be7bb823f32"],"state_sha256":"0bffe419eda247df2bbe798e5c49af68e6ca9780144e8eee923bdc008ced0b6d"}