{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2016:3K37XAXUZ2OJCJMVKPY4PT5XA2","short_pith_number":"pith:3K37XAXU","canonical_record":{"source":{"id":"1608.06886","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-08-24T16:19:42Z","cross_cats_sorted":[],"title_canon_sha256":"8ec7f76d1d699ccd9d9908b8a27e9a9b3b9c8f69b11934603493125521de793c","abstract_canon_sha256":"d1a6dddc2238aec32bfdfdfd576294c4d482a8db63a2383b6761577220efa4b9"},"schema_version":"1.0"},"canonical_sha256":"dab7fb82f4ce9c91259553f1c7cfb706a8aac397184bc2365a647acfee2ed570","source":{"kind":"arxiv","id":"1608.06886","version":3},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.06886","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"arxiv_version","alias_value":"1608.06886v3","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.06886","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"pith_short_12","alias_value":"3K37XAXUZ2OJ","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"3K37XAXUZ2OJCJMV","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"3K37XAXU","created_at":"2026-05-18T12:29:55Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2016:3K37XAXUZ2OJCJMVKPY4PT5XA2","target":"record","payload":{"canonical_record":{"source":{"id":"1608.06886","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-08-24T16:19:42Z","cross_cats_sorted":[],"title_canon_sha256":"8ec7f76d1d699ccd9d9908b8a27e9a9b3b9c8f69b11934603493125521de793c","abstract_canon_sha256":"d1a6dddc2238aec32bfdfdfd576294c4d482a8db63a2383b6761577220efa4b9"},"schema_version":"1.0"},"canonical_sha256":"dab7fb82f4ce9c91259553f1c7cfb706a8aac397184bc2365a647acfee2ed570","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:45:58.661887Z","signature_b64":"KoGQWsJNjIy5XmMCOB5/9zxNQYMawGVbdTTMHVux9R4C7g6suFCgvYER66j8VoM5hkgoO+0MoQQsWt6IFUmSDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dab7fb82f4ce9c91259553f1c7cfb706a8aac397184bc2365a647acfee2ed570","last_reissued_at":"2026-05-18T00:45:58.661396Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:45:58.661396Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1608.06886","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":"2026-05-18T00:45:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"CWQ3lsu81a15US7saGpf4Z7lzLph+pwxSOv4Ia9BGnCHUMHKCExqfi5bug6TH/FKzmPrFMmQPcCvAKDrnHjjBw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T01:39:18.230603Z"},"content_sha256":"4de7bd2a2fbfda0bcd9cf051938938a7d84e9d3b5441423bc8ab730dbca96466","schema_version":"1.0","event_id":"sha256:4de7bd2a2fbfda0bcd9cf051938938a7d84e9d3b5441423bc8ab730dbca96466"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2016:3K37XAXUZ2OJCJMVKPY4PT5XA2","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Behaviour of asymptotically electro-$\\Lambda$ spacetimes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Vee-Liem Saw","submitted_at":"2016-08-24T16:19:42Z","abstract_excerpt":"We present the asymptotic solutions for spacetimes with non-zero cosmological constant $\\Lambda$ coupled to Maxwell fields, using the Newman-Penrose formalism. This extends a recent work that dealt with the vacuum Einstein (Newman-Penrose) equations with $\\Lambda\\neq0$. The results are given in two different null tetrads: the Newman-Unti and Szabados-Tod null tetrads, where the peeling property is exhibited in the former but not the latter. Using these asymptotic solutions, we discuss the mass-loss of an isolated electro-gravitating system with cosmological constant. In a universe with $\\Lambd"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.06886","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":"2026-05-18T00:45:58Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"QE1YPrePbli2jAU1fP8UbYx5aZMknHcmm8ouzruO6tYjIbLp6HD7UcCmzxf0wcCIgRV9Lb7I9oPt25VJrUtBCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-16T01:39:18.231064Z"},"content_sha256":"f870c9bb3eb0f16cc5904b64ee7f6764c5479ca25d55b6ee316ae62d3490403a","schema_version":"1.0","event_id":"sha256:f870c9bb3eb0f16cc5904b64ee7f6764c5479ca25d55b6ee316ae62d3490403a"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/3K37XAXUZ2OJCJMVKPY4PT5XA2/bundle.json","state_url":"https://pith.science/pith/3K37XAXUZ2OJCJMVKPY4PT5XA2/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/3K37XAXUZ2OJCJMVKPY4PT5XA2/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":"2026-08-16T01:39:18Z","links":{"resolver":"https://pith.science/pith/3K37XAXUZ2OJCJMVKPY4PT5XA2","bundle":"https://pith.science/pith/3K37XAXUZ2OJCJMVKPY4PT5XA2/bundle.json","state":"https://pith.science/pith/3K37XAXUZ2OJCJMVKPY4PT5XA2/state.json","well_known_bundle":"https://pith.science/.well-known/pith/3K37XAXUZ2OJCJMVKPY4PT5XA2/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2016:3K37XAXUZ2OJCJMVKPY4PT5XA2","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":"d1a6dddc2238aec32bfdfdfd576294c4d482a8db63a2383b6761577220efa4b9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-08-24T16:19:42Z","title_canon_sha256":"8ec7f76d1d699ccd9d9908b8a27e9a9b3b9c8f69b11934603493125521de793c"},"schema_version":"1.0","source":{"id":"1608.06886","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1608.06886","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"arxiv_version","alias_value":"1608.06886v3","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1608.06886","created_at":"2026-05-18T00:45:58Z"},{"alias_kind":"pith_short_12","alias_value":"3K37XAXUZ2OJ","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_16","alias_value":"3K37XAXUZ2OJCJMV","created_at":"2026-05-18T12:29:55Z"},{"alias_kind":"pith_short_8","alias_value":"3K37XAXU","created_at":"2026-05-18T12:29:55Z"}],"graph_snapshots":[{"event_id":"sha256:f870c9bb3eb0f16cc5904b64ee7f6764c5479ca25d55b6ee316ae62d3490403a","target":"graph","created_at":"2026-05-18T00:45:58Z","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 present the asymptotic solutions for spacetimes with non-zero cosmological constant $\\Lambda$ coupled to Maxwell fields, using the Newman-Penrose formalism. This extends a recent work that dealt with the vacuum Einstein (Newman-Penrose) equations with $\\Lambda\\neq0$. The results are given in two different null tetrads: the Newman-Unti and Szabados-Tod null tetrads, where the peeling property is exhibited in the former but not the latter. Using these asymptotic solutions, we discuss the mass-loss of an isolated electro-gravitating system with cosmological constant. In a universe with $\\Lambd","authors_text":"Vee-Liem Saw","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-08-24T16:19:42Z","title":"Behaviour of asymptotically electro-$\\Lambda$ spacetimes"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1608.06886","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":"sha256:4de7bd2a2fbfda0bcd9cf051938938a7d84e9d3b5441423bc8ab730dbca96466","target":"record","created_at":"2026-05-18T00:45:58Z","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":"d1a6dddc2238aec32bfdfdfd576294c4d482a8db63a2383b6761577220efa4b9","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2016-08-24T16:19:42Z","title_canon_sha256":"8ec7f76d1d699ccd9d9908b8a27e9a9b3b9c8f69b11934603493125521de793c"},"schema_version":"1.0","source":{"id":"1608.06886","kind":"arxiv","version":3}},"canonical_sha256":"dab7fb82f4ce9c91259553f1c7cfb706a8aac397184bc2365a647acfee2ed570","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"dab7fb82f4ce9c91259553f1c7cfb706a8aac397184bc2365a647acfee2ed570","first_computed_at":"2026-05-18T00:45:58.661396Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:45:58.661396Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"KoGQWsJNjIy5XmMCOB5/9zxNQYMawGVbdTTMHVux9R4C7g6suFCgvYER66j8VoM5hkgoO+0MoQQsWt6IFUmSDw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:45:58.661887Z","signed_message":"canonical_sha256_bytes"},"source_id":"1608.06886","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:4de7bd2a2fbfda0bcd9cf051938938a7d84e9d3b5441423bc8ab730dbca96466","sha256:f870c9bb3eb0f16cc5904b64ee7f6764c5479ca25d55b6ee316ae62d3490403a"],"state_sha256":"df22ce072218c79ddb7ed8f09feafdf409886c8c7cdc33f066d2bdcaab8fde63"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cq3bCoQ7VsGgC4W5Hd6ZDhB4atfHZZ9hIfn6mH5H59v6slsrR0dQZ3CRlV6SAKH/FmzLqG6DmdTFONePBbTzCw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-16T01:39:18.234639Z","bundle_sha256":"6afe8c17993aa2eb8738365eb9b76c0e876b821d663bb8ba611568ed59d2d630"}}