{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:5B72KIK3UPG7B2SCIAN2LKZPXQ","short_pith_number":"pith:5B72KIK3","canonical_record":{"source":{"id":"1406.7253","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-06-27T18:04:38Z","cross_cats_sorted":["math-ph","math.AP","math.MP"],"title_canon_sha256":"08d971d2ac4077fb3856d0864785f220500dc8dfee9da4b0619cbc6af83c61de","abstract_canon_sha256":"5f296128d4b2bc406d71f5d2a788138e45531b21173fd433ea9c075beb95a32f"},"schema_version":"1.0"},"canonical_sha256":"e87fa5215ba3cdf0ea42401ba5ab2fbc00d1d627c4875d589a8957f853114b4d","source":{"kind":"arxiv","id":"1406.7253","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.7253","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"arxiv_version","alias_value":"1406.7253v3","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.7253","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"pith_short_12","alias_value":"5B72KIK3UPG7","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"5B72KIK3UPG7B2SC","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"5B72KIK3","created_at":"2026-05-18T12:28:14Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:5B72KIK3UPG7B2SCIAN2LKZPXQ","target":"record","payload":{"canonical_record":{"source":{"id":"1406.7253","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-06-27T18:04:38Z","cross_cats_sorted":["math-ph","math.AP","math.MP"],"title_canon_sha256":"08d971d2ac4077fb3856d0864785f220500dc8dfee9da4b0619cbc6af83c61de","abstract_canon_sha256":"5f296128d4b2bc406d71f5d2a788138e45531b21173fd433ea9c075beb95a32f"},"schema_version":"1.0"},"canonical_sha256":"e87fa5215ba3cdf0ea42401ba5ab2fbc00d1d627c4875d589a8957f853114b4d","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:34:25.722549Z","signature_b64":"BWVNs4vWJdM/JZgPS55R/POD1z0unbQy0WtiJXEgR0ExEMMA63tByQxSVE+RmoVms0bkTtVqtjDTM4r4GUDECQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e87fa5215ba3cdf0ea42401ba5ab2fbc00d1d627c4875d589a8957f853114b4d","last_reissued_at":"2026-05-18T01:34:25.722110Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:34:25.722110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1406.7253","source_version":3,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T01:34:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cimh3GJ6k+dkXcl0CmRvFUadRiN1gTOdnOS9F6+5jyZs+73uwgQy2oaZcMbPQiJd4lNqCaQviqYp+/JF63mPCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T19:28:52.723656Z"},"content_sha256":"cf7c646819cd499358fef5138d0cbede1dbe206f3971ef839ca9de232a14a6e6","schema_version":"1.0","event_id":"sha256:cf7c646819cd499358fef5138d0cbede1dbe206f3971ef839ca9de232a14a6e6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:5B72KIK3UPG7B2SCIAN2LKZPXQ","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"On the global uniqueness for the Einstein-Maxwell-scalar field system with a cosmological constant. Part 2: Structure of the solutions and stability of the Cauchy horizon","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.AP","math.MP"],"primary_cat":"gr-qc","authors_text":"Jo\\~ao L. Costa, Jorge Drumond Silva, Jos\\'e Nat\\'ario, Pedro M. Gir\\~ao","submitted_at":"2014-06-27T18:04:38Z","abstract_excerpt":"This paper is the second part of a trilogy dedicated to the following problem: given spherically symmetric characteristic initial data for the Einstein-Maxwell-scalar field system with a cosmological constant $\\Lambda$, with the data on the outgoing initial null hypersurface given by a subextremal Reissner-Nordstrom black hole event horizon, study the future extendibility of the corresponding maximal globally hyperbolic development as a \"suitably regular\" Lorentzian manifold.\n  In the first paper of this sequence, we established well posedness of the characteristic problem with general initial"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.7253","kind":"arxiv","version":3},"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":"2026-05-18T01:34:25Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"uBO3thh0Csmla9IYFMScKzT150y84Y6CSm29wdQp6qUEaqcTttvoLs+laPx9ZAbTyodteSYH3moaXVeXrvUcDw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-04T19:28:52.724208Z"},"content_sha256":"6950651c240900cd0ebc0fb744356d5579cff098413a222e9b07b4cb9bab4905","schema_version":"1.0","event_id":"sha256:6950651c240900cd0ebc0fb744356d5579cff098413a222e9b07b4cb9bab4905"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5B72KIK3UPG7B2SCIAN2LKZPXQ/bundle.json","state_url":"https://pith.science/pith/5B72KIK3UPG7B2SCIAN2LKZPXQ/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5B72KIK3UPG7B2SCIAN2LKZPXQ/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":"2026-06-04T19:28:52Z","links":{"resolver":"https://pith.science/pith/5B72KIK3UPG7B2SCIAN2LKZPXQ","bundle":"https://pith.science/pith/5B72KIK3UPG7B2SCIAN2LKZPXQ/bundle.json","state":"https://pith.science/pith/5B72KIK3UPG7B2SCIAN2LKZPXQ/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5B72KIK3UPG7B2SCIAN2LKZPXQ/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:5B72KIK3UPG7B2SCIAN2LKZPXQ","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":"5f296128d4b2bc406d71f5d2a788138e45531b21173fd433ea9c075beb95a32f","cross_cats_sorted":["math-ph","math.AP","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-06-27T18:04:38Z","title_canon_sha256":"08d971d2ac4077fb3856d0864785f220500dc8dfee9da4b0619cbc6af83c61de"},"schema_version":"1.0","source":{"id":"1406.7253","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1406.7253","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"arxiv_version","alias_value":"1406.7253v3","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1406.7253","created_at":"2026-05-18T01:34:25Z"},{"alias_kind":"pith_short_12","alias_value":"5B72KIK3UPG7","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_16","alias_value":"5B72KIK3UPG7B2SC","created_at":"2026-05-18T12:28:14Z"},{"alias_kind":"pith_short_8","alias_value":"5B72KIK3","created_at":"2026-05-18T12:28:14Z"}],"graph_snapshots":[{"event_id":"sha256:6950651c240900cd0ebc0fb744356d5579cff098413a222e9b07b4cb9bab4905","target":"graph","created_at":"2026-05-18T01:34:25Z","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":"This paper is the second part of a trilogy dedicated to the following problem: given spherically symmetric characteristic initial data for the Einstein-Maxwell-scalar field system with a cosmological constant $\\Lambda$, with the data on the outgoing initial null hypersurface given by a subextremal Reissner-Nordstrom black hole event horizon, study the future extendibility of the corresponding maximal globally hyperbolic development as a \"suitably regular\" Lorentzian manifold.\n  In the first paper of this sequence, we established well posedness of the characteristic problem with general initial","authors_text":"Jo\\~ao L. Costa, Jorge Drumond Silva, Jos\\'e Nat\\'ario, Pedro M. Gir\\~ao","cross_cats":["math-ph","math.AP","math.MP"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-06-27T18:04:38Z","title":"On the global uniqueness for the Einstein-Maxwell-scalar field system with a cosmological constant. Part 2: Structure of the solutions and stability of the Cauchy horizon"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1406.7253","kind":"arxiv","version":3},"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:cf7c646819cd499358fef5138d0cbede1dbe206f3971ef839ca9de232a14a6e6","target":"record","created_at":"2026-05-18T01:34:25Z","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":"5f296128d4b2bc406d71f5d2a788138e45531b21173fd433ea9c075beb95a32f","cross_cats_sorted":["math-ph","math.AP","math.MP"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-06-27T18:04:38Z","title_canon_sha256":"08d971d2ac4077fb3856d0864785f220500dc8dfee9da4b0619cbc6af83c61de"},"schema_version":"1.0","source":{"id":"1406.7253","kind":"arxiv","version":3}},"canonical_sha256":"e87fa5215ba3cdf0ea42401ba5ab2fbc00d1d627c4875d589a8957f853114b4d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e87fa5215ba3cdf0ea42401ba5ab2fbc00d1d627c4875d589a8957f853114b4d","first_computed_at":"2026-05-18T01:34:25.722110Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:34:25.722110Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BWVNs4vWJdM/JZgPS55R/POD1z0unbQy0WtiJXEgR0ExEMMA63tByQxSVE+RmoVms0bkTtVqtjDTM4r4GUDECQ==","signature_status":"signed_v1","signed_at":"2026-05-18T01:34:25.722549Z","signed_message":"canonical_sha256_bytes"},"source_id":"1406.7253","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:cf7c646819cd499358fef5138d0cbede1dbe206f3971ef839ca9de232a14a6e6","sha256:6950651c240900cd0ebc0fb744356d5579cff098413a222e9b07b4cb9bab4905"],"state_sha256":"3e88886eacbc1f4f3d74e7c23c5b1310fa7234421ae271ce89352c87ee73cfa4"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"u/dJZkAyNzJ/IF13kd2G9NRIxgDBVW6rWCPLkDYvmpdVGUqTtLxLF0v462ixSBD/iecD3BGaR0bFSA3nwlFXDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-04T19:28:52.726952Z","bundle_sha256":"bc399fba325da9c6599c6252c540cbf5bbc289817e70693b4ef2b14ca31ac927"}}