{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2013:5UJ4KJASL3XKBO4HF3QXUWI7ZW","short_pith_number":"pith:5UJ4KJAS","canonical_record":{"source":{"id":"1303.7385","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-03-29T13:04:09Z","cross_cats_sorted":[],"title_canon_sha256":"8d58459a4a1449481d58410fb102de94de664b92ea52613fe19433c04cdd133a","abstract_canon_sha256":"29a640d8205c491a9114281b78f6803db88f57dedca0a89cc55577172996d942"},"schema_version":"1.0"},"canonical_sha256":"ed13c524125eeea0bb872ee17a591fcd87442eae549de125f681cbcbd3becc55","source":{"kind":"arxiv","id":"1303.7385","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.7385","created_at":"2026-05-18T03:08:47Z"},{"alias_kind":"arxiv_version","alias_value":"1303.7385v1","created_at":"2026-05-18T03:08:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.7385","created_at":"2026-05-18T03:08:47Z"},{"alias_kind":"pith_short_12","alias_value":"5UJ4KJASL3XK","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5UJ4KJASL3XKBO4H","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5UJ4KJAS","created_at":"2026-05-18T12:27:34Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2013:5UJ4KJASL3XKBO4HF3QXUWI7ZW","target":"record","payload":{"canonical_record":{"source":{"id":"1303.7385","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-03-29T13:04:09Z","cross_cats_sorted":[],"title_canon_sha256":"8d58459a4a1449481d58410fb102de94de664b92ea52613fe19433c04cdd133a","abstract_canon_sha256":"29a640d8205c491a9114281b78f6803db88f57dedca0a89cc55577172996d942"},"schema_version":"1.0"},"canonical_sha256":"ed13c524125eeea0bb872ee17a591fcd87442eae549de125f681cbcbd3becc55","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:08:47.223546Z","signature_b64":"j9NPL0EBysJIts3kRSZweRQtGTNdkcVW/ceFb+ZK3wvIRcS2XyPKTuIvmbkTYoIwKNpTQVktN5YF6FLWx3NXAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ed13c524125eeea0bb872ee17a591fcd87442eae549de125f681cbcbd3becc55","last_reissued_at":"2026-05-18T03:08:47.222825Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:08:47.222825Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1303.7385","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":"2026-05-18T03:08:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"/RmhBJEO3epSu/X41jCV3S6KuiwCBBjiqAQDTWd2G+sb8J/7Bpp9Evkk0JURELLqEj+y/Y6lVbViH6oAXcriBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T18:22:03.243678Z"},"content_sha256":"fe2808f60e9b8402ce31a870d28a746a2ebe7c2463d8267084ac10f7c971e4ae","schema_version":"1.0","event_id":"sha256:fe2808f60e9b8402ce31a870d28a746a2ebe7c2463d8267084ac10f7c971e4ae"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2013:5UJ4KJASL3XKBO4HF3QXUWI7ZW","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The radiative self-force and charged fluids","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.plasm-ph","authors_text":"A. Carr, A. Noble, D.A. Burton, J. Gratus","submitted_at":"2013-03-29T13:04:09Z","abstract_excerpt":"We develop a new fluid model of a warm plasma that includes the radiative self-force on each plasma electron. Our approach is a natural generalization of established methods for generating fluid models without radiation reaction. The equilibrium of a magnetized plasma is analysed, and it is shown that the thermal motion is confined to the magnetic field lines. A dispersion relation is deduced for electric waves in a magnetized plasma, and it is shown to agree with our recently established relativistic kinetic theory derived from the Lorentz-Abraham-Dirac equation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.7385","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":"2026-05-18T03:08:47Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"c4zNW5dfmXj9rVVMSNSRlt7ApqmdyZbuxi3oDyLscNITcmXZMfCi7bm4qG9K8pr9aQ7UZHPysGqZBUuSSEymBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-08T18:22:03.244384Z"},"content_sha256":"59800a53fbf5e99dc7e7f43ab51c8d404d66a67aab4aa68221cef600ff62fd38","schema_version":"1.0","event_id":"sha256:59800a53fbf5e99dc7e7f43ab51c8d404d66a67aab4aa68221cef600ff62fd38"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/5UJ4KJASL3XKBO4HF3QXUWI7ZW/bundle.json","state_url":"https://pith.science/pith/5UJ4KJASL3XKBO4HF3QXUWI7ZW/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/5UJ4KJASL3XKBO4HF3QXUWI7ZW/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":"2026-06-08T18:22:03Z","links":{"resolver":"https://pith.science/pith/5UJ4KJASL3XKBO4HF3QXUWI7ZW","bundle":"https://pith.science/pith/5UJ4KJASL3XKBO4HF3QXUWI7ZW/bundle.json","state":"https://pith.science/pith/5UJ4KJASL3XKBO4HF3QXUWI7ZW/state.json","well_known_bundle":"https://pith.science/.well-known/pith/5UJ4KJASL3XKBO4HF3QXUWI7ZW/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2013:5UJ4KJASL3XKBO4HF3QXUWI7ZW","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":"29a640d8205c491a9114281b78f6803db88f57dedca0a89cc55577172996d942","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-03-29T13:04:09Z","title_canon_sha256":"8d58459a4a1449481d58410fb102de94de664b92ea52613fe19433c04cdd133a"},"schema_version":"1.0","source":{"id":"1303.7385","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1303.7385","created_at":"2026-05-18T03:08:47Z"},{"alias_kind":"arxiv_version","alias_value":"1303.7385v1","created_at":"2026-05-18T03:08:47Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1303.7385","created_at":"2026-05-18T03:08:47Z"},{"alias_kind":"pith_short_12","alias_value":"5UJ4KJASL3XK","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_16","alias_value":"5UJ4KJASL3XKBO4H","created_at":"2026-05-18T12:27:34Z"},{"alias_kind":"pith_short_8","alias_value":"5UJ4KJAS","created_at":"2026-05-18T12:27:34Z"}],"graph_snapshots":[{"event_id":"sha256:59800a53fbf5e99dc7e7f43ab51c8d404d66a67aab4aa68221cef600ff62fd38","target":"graph","created_at":"2026-05-18T03:08:47Z","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 develop a new fluid model of a warm plasma that includes the radiative self-force on each plasma electron. Our approach is a natural generalization of established methods for generating fluid models without radiation reaction. The equilibrium of a magnetized plasma is analysed, and it is shown that the thermal motion is confined to the magnetic field lines. A dispersion relation is deduced for electric waves in a magnetized plasma, and it is shown to agree with our recently established relativistic kinetic theory derived from the Lorentz-Abraham-Dirac equation.","authors_text":"A. Carr, A. Noble, D.A. Burton, J. Gratus","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-03-29T13:04:09Z","title":"The radiative self-force and charged fluids"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1303.7385","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:fe2808f60e9b8402ce31a870d28a746a2ebe7c2463d8267084ac10f7c971e4ae","target":"record","created_at":"2026-05-18T03:08:47Z","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":"29a640d8205c491a9114281b78f6803db88f57dedca0a89cc55577172996d942","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.plasm-ph","submitted_at":"2013-03-29T13:04:09Z","title_canon_sha256":"8d58459a4a1449481d58410fb102de94de664b92ea52613fe19433c04cdd133a"},"schema_version":"1.0","source":{"id":"1303.7385","kind":"arxiv","version":1}},"canonical_sha256":"ed13c524125eeea0bb872ee17a591fcd87442eae549de125f681cbcbd3becc55","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ed13c524125eeea0bb872ee17a591fcd87442eae549de125f681cbcbd3becc55","first_computed_at":"2026-05-18T03:08:47.222825Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T03:08:47.222825Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"j9NPL0EBysJIts3kRSZweRQtGTNdkcVW/ceFb+ZK3wvIRcS2XyPKTuIvmbkTYoIwKNpTQVktN5YF6FLWx3NXAA==","signature_status":"signed_v1","signed_at":"2026-05-18T03:08:47.223546Z","signed_message":"canonical_sha256_bytes"},"source_id":"1303.7385","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:fe2808f60e9b8402ce31a870d28a746a2ebe7c2463d8267084ac10f7c971e4ae","sha256:59800a53fbf5e99dc7e7f43ab51c8d404d66a67aab4aa68221cef600ff62fd38"],"state_sha256":"834b7d9970a3a786952c128a81efc244a974800b7b429128394dc7b623c11c8a"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hEHU6y5ASTe1oIiHF1YDQ389uEEwzd4l7pI7qluKe/mT2GwlmLddB01oo5pNTl+rJvng9e9YlgxE+yZyun/aAQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-08T18:22:03.248460Z","bundle_sha256":"cbe990b9e092a4bd336626a0f90c351f2cd283eac294448790e13126abb64988"}}