{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:YKOIX6NZTKLF5OJXKRZSWIK6RA","short_pith_number":"pith:YKOIX6NZ","canonical_record":{"source":{"id":"1410.3148","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-10-12T20:55:49Z","cross_cats_sorted":[],"title_canon_sha256":"a5aa16fb462e730f1528ab3b934f20ac84550e5113ed60debb7b401a3facb1d7","abstract_canon_sha256":"adc5f9c5f9eb94467bd55d0d4b892af70996fc70ff764378662b256b0f9f3320"},"schema_version":"1.0"},"canonical_sha256":"c29c8bf9b99a965eb93754732b215e882325e128ffa74f420b892f483639a677","source":{"kind":"arxiv","id":"1410.3148","version":4},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.3148","created_at":"2026-05-18T02:18:49Z"},{"alias_kind":"arxiv_version","alias_value":"1410.3148v4","created_at":"2026-05-18T02:18:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.3148","created_at":"2026-05-18T02:18:49Z"},{"alias_kind":"pith_short_12","alias_value":"YKOIX6NZTKLF","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"YKOIX6NZTKLF5OJX","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"YKOIX6NZ","created_at":"2026-05-18T12:28:57Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:YKOIX6NZTKLF5OJXKRZSWIK6RA","target":"record","payload":{"canonical_record":{"source":{"id":"1410.3148","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-10-12T20:55:49Z","cross_cats_sorted":[],"title_canon_sha256":"a5aa16fb462e730f1528ab3b934f20ac84550e5113ed60debb7b401a3facb1d7","abstract_canon_sha256":"adc5f9c5f9eb94467bd55d0d4b892af70996fc70ff764378662b256b0f9f3320"},"schema_version":"1.0"},"canonical_sha256":"c29c8bf9b99a965eb93754732b215e882325e128ffa74f420b892f483639a677","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:49.416164Z","signature_b64":"nB3TC4Pvx+xlVPKXlNo01gus5aNsd2hR+azdlDCxXglvC/MLj6HtYDSO/4/JdqRKqUj5IeRJ0xONPuUm7snFBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"c29c8bf9b99a965eb93754732b215e882325e128ffa74f420b892f483639a677","last_reissued_at":"2026-05-18T02:18:49.415532Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:49.415532Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1410.3148","source_version":4,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:18:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YW+jmsTJKo1PwwBNAO0E2hx6q6ZFDJMxDsTQxCSwoZzGIo01XkgaAgRGoqslsEWHfi2JVCB4hWbOlORfMpjNCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T10:15:17.694023Z"},"content_sha256":"c4e350250bfe8639e4f2a0897fa4cdd7291233fd61bacafbd869de9b03bd5dbf","schema_version":"1.0","event_id":"sha256:c4e350250bfe8639e4f2a0897fa4cdd7291233fd61bacafbd869de9b03bd5dbf"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:YKOIX6NZTKLF5OJXKRZSWIK6RA","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Conformastationary disk-haloes in Einstein-Maxwell gravity","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"gr-qc","authors_text":"Antonio C. Guti\\'errez-Pi\\~neres","submitted_at":"2014-10-12T20:55:49Z","abstract_excerpt":"An exact solution of the Einstein-Maxwell field equations for a conformastationary metric with magnetized disk-haloes sources is worked out in full. The characterization of the nature of the energy momentum tensor of the source is discussed. All the expressions are presented in terms of a solution of the Laplace's equation. A \"generalization\" of the Kuzmin solution of the Laplace's equations is used as a particular example. The solution obtained is asymptotically flat in general and turns out to be free of singularities. All the relevant quantities show a reasonable physical behaviour."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.3148","kind":"arxiv","version":4},"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":"2026-05-18T02:18:49Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"cTZ42cjiwfEEEhQZjdr1FKwozUz+BDW1rmybAbBgsX1ttk+iUL2/UTQzomS2GQD6WxdDPeJvzm1vUIry3BBfCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-12T10:15:17.694578Z"},"content_sha256":"162722891ad8b74ea56556ada6085fc6204aa0545a0bbf11c262a411b7557c31","schema_version":"1.0","event_id":"sha256:162722891ad8b74ea56556ada6085fc6204aa0545a0bbf11c262a411b7557c31"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/YKOIX6NZTKLF5OJXKRZSWIK6RA/bundle.json","state_url":"https://pith.science/pith/YKOIX6NZTKLF5OJXKRZSWIK6RA/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/YKOIX6NZTKLF5OJXKRZSWIK6RA/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":"2026-06-12T10:15:17Z","links":{"resolver":"https://pith.science/pith/YKOIX6NZTKLF5OJXKRZSWIK6RA","bundle":"https://pith.science/pith/YKOIX6NZTKLF5OJXKRZSWIK6RA/bundle.json","state":"https://pith.science/pith/YKOIX6NZTKLF5OJXKRZSWIK6RA/state.json","well_known_bundle":"https://pith.science/.well-known/pith/YKOIX6NZTKLF5OJXKRZSWIK6RA/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:YKOIX6NZTKLF5OJXKRZSWIK6RA","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":"adc5f9c5f9eb94467bd55d0d4b892af70996fc70ff764378662b256b0f9f3320","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-10-12T20:55:49Z","title_canon_sha256":"a5aa16fb462e730f1528ab3b934f20ac84550e5113ed60debb7b401a3facb1d7"},"schema_version":"1.0","source":{"id":"1410.3148","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1410.3148","created_at":"2026-05-18T02:18:49Z"},{"alias_kind":"arxiv_version","alias_value":"1410.3148v4","created_at":"2026-05-18T02:18:49Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1410.3148","created_at":"2026-05-18T02:18:49Z"},{"alias_kind":"pith_short_12","alias_value":"YKOIX6NZTKLF","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_16","alias_value":"YKOIX6NZTKLF5OJX","created_at":"2026-05-18T12:28:57Z"},{"alias_kind":"pith_short_8","alias_value":"YKOIX6NZ","created_at":"2026-05-18T12:28:57Z"}],"graph_snapshots":[{"event_id":"sha256:162722891ad8b74ea56556ada6085fc6204aa0545a0bbf11c262a411b7557c31","target":"graph","created_at":"2026-05-18T02:18:49Z","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":"An exact solution of the Einstein-Maxwell field equations for a conformastationary metric with magnetized disk-haloes sources is worked out in full. The characterization of the nature of the energy momentum tensor of the source is discussed. All the expressions are presented in terms of a solution of the Laplace's equation. A \"generalization\" of the Kuzmin solution of the Laplace's equations is used as a particular example. The solution obtained is asymptotically flat in general and turns out to be free of singularities. All the relevant quantities show a reasonable physical behaviour.","authors_text":"Antonio C. Guti\\'errez-Pi\\~neres","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-10-12T20:55:49Z","title":"Conformastationary disk-haloes in Einstein-Maxwell gravity"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1410.3148","kind":"arxiv","version":4},"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:c4e350250bfe8639e4f2a0897fa4cdd7291233fd61bacafbd869de9b03bd5dbf","target":"record","created_at":"2026-05-18T02:18:49Z","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":"adc5f9c5f9eb94467bd55d0d4b892af70996fc70ff764378662b256b0f9f3320","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2014-10-12T20:55:49Z","title_canon_sha256":"a5aa16fb462e730f1528ab3b934f20ac84550e5113ed60debb7b401a3facb1d7"},"schema_version":"1.0","source":{"id":"1410.3148","kind":"arxiv","version":4}},"canonical_sha256":"c29c8bf9b99a965eb93754732b215e882325e128ffa74f420b892f483639a677","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"c29c8bf9b99a965eb93754732b215e882325e128ffa74f420b892f483639a677","first_computed_at":"2026-05-18T02:18:49.415532Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:18:49.415532Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"nB3TC4Pvx+xlVPKXlNo01gus5aNsd2hR+azdlDCxXglvC/MLj6HtYDSO/4/JdqRKqUj5IeRJ0xONPuUm7snFBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:18:49.416164Z","signed_message":"canonical_sha256_bytes"},"source_id":"1410.3148","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c4e350250bfe8639e4f2a0897fa4cdd7291233fd61bacafbd869de9b03bd5dbf","sha256:162722891ad8b74ea56556ada6085fc6204aa0545a0bbf11c262a411b7557c31"],"state_sha256":"8337772dfd57ee52408d1f0f670ba101fe4655bdbe9226a2cfdb6c63988d9cd8"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"D9ZrALe0Hej538fcgMmY3rcmEjzIFkTk7Ch81TQZ10GOqC4WFdMrGY3M6NodHDCkPErHIs+wGDUn6hl1SjZJAg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-12T10:15:17.697085Z","bundle_sha256":"815b09b5c3376aafe0c2a73edc7cef1e2dfc25548bc45f5d5e757c91f8a233d7"}}