{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:5ZR53UUBPE3CK7CJTDGS7EWJZV","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":"462845f308e075222a24830025110765cfe9bdfbfb37525a85efdde73ac5acb0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2026-02-27T17:25:59Z","title_canon_sha256":"74b35089926e42afedf631df70a4f19303bb08abba0d83355079ea68ad7dd55d"},"schema_version":"1.0","source":{"id":"2603.00219","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2603.00219","created_at":"2026-05-25T02:01:16Z"},{"alias_kind":"arxiv_version","alias_value":"2603.00219v2","created_at":"2026-05-25T02:01:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.00219","created_at":"2026-05-25T02:01:16Z"},{"alias_kind":"pith_short_12","alias_value":"5ZR53UUBPE3C","created_at":"2026-05-25T02:01:16Z"},{"alias_kind":"pith_short_16","alias_value":"5ZR53UUBPE3CK7CJ","created_at":"2026-05-25T02:01:16Z"},{"alias_kind":"pith_short_8","alias_value":"5ZR53UUB","created_at":"2026-05-25T02:01:16Z"}],"graph_snapshots":[{"event_id":"sha256:9b0170947935e15b2db408e9a9cb4528fff9089b7e60141ea1f0ca0454ab0dfa","target":"graph","created_at":"2026-05-25T02:01:16Z","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"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2603.00219/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The non-relativistic Goedecke equation (1975), which describes the motion of a point charge taking into account the radiation reaction, has no \"runaway\" solutions. A \"physical\" method of covariant generalization of this equation is proposed, a special case of which is based on the Lorentz transformations in a coordinate--free covariant representation. Two equivalent forms of a new classical relativistic equation of motion of a point charge are obtained. It is shown that the Abraham--Lorentz--Dirac (ALD) and the Mo--Papas (MP) equations are approximate consequences of the presented theory.","authors_text":"Anatoliy V. Sermyagin (JSC \"Institute in Physical-Technical Problems\", Dubna, Russia)","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2026-02-27T17:25:59Z","title":"Still The New Classical Relativistic Equation of Charge Motion in an Electromagnetic Field"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.00219","kind":"arxiv","version":2},"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":"sha256:30ff1783ddead6e14b34d38ebde07d781ae8382698f7a687e1e336c381d7f77b","target":"record","created_at":"2026-05-25T02:01:16Z","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":"462845f308e075222a24830025110765cfe9bdfbfb37525a85efdde73ac5acb0","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2026-02-27T17:25:59Z","title_canon_sha256":"74b35089926e42afedf631df70a4f19303bb08abba0d83355079ea68ad7dd55d"},"schema_version":"1.0","source":{"id":"2603.00219","kind":"arxiv","version":2}},"canonical_sha256":"ee63ddd2817936257c4998cd2f92c9cd718e680bd76a0bc86edce963dddbe175","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"ee63ddd2817936257c4998cd2f92c9cd718e680bd76a0bc86edce963dddbe175","first_computed_at":"2026-05-25T02:01:16.276135Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-25T02:01:16.276135Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"eP3ZUuRnW9cSNBH4G8Cu88h0Z4p0Sfoso5kqZvkoaq/iX+LbxsE9VbmGgLcT7u3fmhh032U5OxU1NCQTCRggBA==","signature_status":"signed_v1","signed_at":"2026-05-25T02:01:16.276773Z","signed_message":"canonical_sha256_bytes"},"source_id":"2603.00219","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:30ff1783ddead6e14b34d38ebde07d781ae8382698f7a687e1e336c381d7f77b","sha256:9b0170947935e15b2db408e9a9cb4528fff9089b7e60141ea1f0ca0454ab0dfa"],"state_sha256":"32cd535b74436f4bcd9f1acc433d9d0848b77fd7537d599a0bee6414af2f37c6"}