{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2012:ZJCL67Q3XGZNXRLG54HFXTXQCF","short_pith_number":"pith:ZJCL67Q3","canonical_record":{"source":{"id":"1212.0130","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2012-12-01T16:38:55Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"d5850a05bb5c4233ed75ead3e6817937e4060936e073e0a148a3d4eff32bedf4","abstract_canon_sha256":"d3edae2b958ea1cde3cb63d481fd1107269c363ecf5faf0a948aaa73831d6092"},"schema_version":"1.0"},"canonical_sha256":"ca44bf7e1bb9b2dbc566ef0e5bcef01168f457c04e76d7e440ba381b15169a90","source":{"kind":"arxiv","id":"1212.0130","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.0130","created_at":"2026-05-18T03:13:34Z"},{"alias_kind":"arxiv_version","alias_value":"1212.0130v1","created_at":"2026-05-18T03:13:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.0130","created_at":"2026-05-18T03:13:34Z"},{"alias_kind":"pith_short_12","alias_value":"ZJCL67Q3XGZN","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"ZJCL67Q3XGZNXRLG","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"ZJCL67Q3","created_at":"2026-05-18T12:27:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2012:ZJCL67Q3XGZNXRLG54HFXTXQCF","target":"record","payload":{"canonical_record":{"source":{"id":"1212.0130","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2012-12-01T16:38:55Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"d5850a05bb5c4233ed75ead3e6817937e4060936e073e0a148a3d4eff32bedf4","abstract_canon_sha256":"d3edae2b958ea1cde3cb63d481fd1107269c363ecf5faf0a948aaa73831d6092"},"schema_version":"1.0"},"canonical_sha256":"ca44bf7e1bb9b2dbc566ef0e5bcef01168f457c04e76d7e440ba381b15169a90","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:13:34.108546Z","signature_b64":"jNTbYtNXd7zeMHribLZXom3h8gKibZ+oPdxLrWc9ni8yf4vBdhyXCUpo7wE81zNFmTZhzrxL/+NsW9ZwtjymAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca44bf7e1bb9b2dbc566ef0e5bcef01168f457c04e76d7e440ba381b15169a90","last_reissued_at":"2026-05-18T03:13:34.107760Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:13:34.107760Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1212.0130","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T03:13:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"O3p9rQAHuZ7ufBUJZKfDC9h3oDpBnjMjXoU0quQKtrSUXuMvBz+6lHle5rhGEKnyIHkJFM9KUEVYuLFtJ8IaDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T10:51:42.308962Z"},"content_sha256":"15e47627910594eb8161a81bde84882016073e784d1c8533236eeadcd9d876ce","schema_version":"1.0","event_id":"sha256:15e47627910594eb8161a81bde84882016073e784d1c8533236eeadcd9d876ce"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2012:ZJCL67Q3XGZNXRLG54HFXTXQCF","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Modeling magnetized neutron stars using resistive MHD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"astro-ph.HE","authors_text":"Carlos Palenzuela","submitted_at":"2012-12-01T16:38:55Z","abstract_excerpt":"This work presents an implementation of the resistive MHD equations for a generic algebraic Ohm's law which includes the effects of finite resistivity within full General Relativity. The implementation naturally accounts for magnetic-field-induced anisotropies and, by adopting a phenomenological current, is able to accurately describe electromagnetic fields in the star and in its magnetosphere. We illustrate the application of this approach in interesting systems with astrophysical implications; the aligned rotator solution and the collapse of a magnetized rotating neutron star to a black hole"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.0130","kind":"arxiv","version":1},"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":"2026-05-18T03:13:34Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sWO6LejldF2VJHDvrO1EtEhWBoThhF9USxq6Zr53QiQVQtTeRiIzm+VE4JUBii+JUgJzFSAi3kyhJ3O4CBPoAw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-11T10:51:42.309592Z"},"content_sha256":"142b696a80b49f1814f1e6db38ccc16b04886208fe7d577d9fb90d0ab0b7ea32","schema_version":"1.0","event_id":"sha256:142b696a80b49f1814f1e6db38ccc16b04886208fe7d577d9fb90d0ab0b7ea32"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/ZJCL67Q3XGZNXRLG54HFXTXQCF/bundle.json","state_url":"https://pith.science/pith/ZJCL67Q3XGZNXRLG54HFXTXQCF/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/ZJCL67Q3XGZNXRLG54HFXTXQCF/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":"2026-06-11T10:51:42Z","links":{"resolver":"https://pith.science/pith/ZJCL67Q3XGZNXRLG54HFXTXQCF","bundle":"https://pith.science/pith/ZJCL67Q3XGZNXRLG54HFXTXQCF/bundle.json","state":"https://pith.science/pith/ZJCL67Q3XGZNXRLG54HFXTXQCF/state.json","well_known_bundle":"https://pith.science/.well-known/pith/ZJCL67Q3XGZNXRLG54HFXTXQCF/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2012:ZJCL67Q3XGZNXRLG54HFXTXQCF","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":"d3edae2b958ea1cde3cb63d481fd1107269c363ecf5faf0a948aaa73831d6092","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2012-12-01T16:38:55Z","title_canon_sha256":"d5850a05bb5c4233ed75ead3e6817937e4060936e073e0a148a3d4eff32bedf4"},"schema_version":"1.0","source":{"id":"1212.0130","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1212.0130","created_at":"2026-05-18T03:13:34Z"},{"alias_kind":"arxiv_version","alias_value":"1212.0130v1","created_at":"2026-05-18T03:13:34Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.0130","created_at":"2026-05-18T03:13:34Z"},{"alias_kind":"pith_short_12","alias_value":"ZJCL67Q3XGZN","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_16","alias_value":"ZJCL67Q3XGZNXRLG","created_at":"2026-05-18T12:27:30Z"},{"alias_kind":"pith_short_8","alias_value":"ZJCL67Q3","created_at":"2026-05-18T12:27:30Z"}],"graph_snapshots":[{"event_id":"sha256:142b696a80b49f1814f1e6db38ccc16b04886208fe7d577d9fb90d0ab0b7ea32","target":"graph","created_at":"2026-05-18T03:13:34Z","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 work presents an implementation of the resistive MHD equations for a generic algebraic Ohm's law which includes the effects of finite resistivity within full General Relativity. The implementation naturally accounts for magnetic-field-induced anisotropies and, by adopting a phenomenological current, is able to accurately describe electromagnetic fields in the star and in its magnetosphere. We illustrate the application of this approach in interesting systems with astrophysical implications; the aligned rotator solution and the collapse of a magnetized rotating neutron star to a black hole","authors_text":"Carlos Palenzuela","cross_cats":["gr-qc"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2012-12-01T16:38:55Z","title":"Modeling magnetized neutron stars using resistive MHD"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.0130","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":"sha256:15e47627910594eb8161a81bde84882016073e784d1c8533236eeadcd9d876ce","target":"record","created_at":"2026-05-18T03:13:34Z","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":"d3edae2b958ea1cde3cb63d481fd1107269c363ecf5faf0a948aaa73831d6092","cross_cats_sorted":["gr-qc"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"astro-ph.HE","submitted_at":"2012-12-01T16:38:55Z","title_canon_sha256":"d5850a05bb5c4233ed75ead3e6817937e4060936e073e0a148a3d4eff32bedf4"},"schema_version":"1.0","source":{"id":"1212.0130","kind":"arxiv","version":1}},"canonical_sha256":"ca44bf7e1bb9b2dbc566ef0e5bcef01168f457c04e76d7e440ba381b15169a90","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ca44bf7e1bb9b2dbc566ef0e5bcef01168f457c04e76d7e440ba381b15169a90","first_computed_at":"2026-05-18T03:13:34.107760Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:13:34.107760Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"jNTbYtNXd7zeMHribLZXom3h8gKibZ+oPdxLrWc9ni8yf4vBdhyXCUpo7wE81zNFmTZhzrxL/+NsW9ZwtjymAQ==","signature_status":"signed_v1","signed_at":"2026-05-18T03:13:34.108546Z","signed_message":"canonical_sha256_bytes"},"source_id":"1212.0130","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:15e47627910594eb8161a81bde84882016073e784d1c8533236eeadcd9d876ce","sha256:142b696a80b49f1814f1e6db38ccc16b04886208fe7d577d9fb90d0ab0b7ea32"],"state_sha256":"a9b763c12efd13c7c3498c400181a5e8b72aa4df6bdf28def1dd7af265d3489c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"VuA8UHakxMlG9iy7u+X4R5EajIRQDvH91DFCzKR+mvOluP7kmiuz48/wq/BDmEGnS9gOTQPx4RxDYOg+tyLnAw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-11T10:51:42.312683Z","bundle_sha256":"3cc0bac9c5a9c401a67164434e6a020e69935fd7a848a8887e0027784b131acc"}}