{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:CLHZW6CNR7YELQ7HHD3HWN342S","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":"622629101353eac821c89285445a421d8d019cbe8c5757853f5e471673c5694f","cross_cats_sorted":["hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2022-12-20T18:04:17Z","title_canon_sha256":"def272b50908fce615fe6a6ee902398de2088b2b92452231e092cb3dfa7ced14"},"schema_version":"1.0","source":{"id":"2212.10486","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2212.10486","created_at":"2026-07-05T06:31:07Z"},{"alias_kind":"arxiv_version","alias_value":"2212.10486v1","created_at":"2026-07-05T06:31:07Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2212.10486","created_at":"2026-07-05T06:31:07Z"},{"alias_kind":"pith_short_12","alias_value":"CLHZW6CNR7YE","created_at":"2026-07-05T06:31:07Z"},{"alias_kind":"pith_short_16","alias_value":"CLHZW6CNR7YELQ7H","created_at":"2026-07-05T06:31:07Z"},{"alias_kind":"pith_short_8","alias_value":"CLHZW6CN","created_at":"2026-07-05T06:31:07Z"}],"graph_snapshots":[{"event_id":"sha256:f56d718574153e00e495972a3527206e3d9dff11b642a771a3ef3317747e783f","target":"graph","created_at":"2026-07-05T06:31:07Z","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/2212.10486/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In recent years, significant progress has been made in the computation of conservative and dissipative scattering observables using the post-Minkowskian approach to gravitational dynamics. However, for accurate modeling of unbound orbits, an appropriate effective-one-body (EOB) resummation of the post-Minkowski results that also accounts for dissipative dynamics is desirable. As a step in this direction, we consider the electromagnetic analog of this problem here. We show that a six-parameter equation of motion encapsulates the effective-one-body dynamics for the electromagnetic scattering pro","authors_text":"Karthik Rajeev, S. Shankaranarayanan","cross_cats":["hep-th"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2022-12-20T18:04:17Z","title":"Effective-one-body formalism for leading-order radiative effects in the post-linear framework"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2212.10486","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:b412a7f7e856dac27ff96c95cd6bda9dafea0ca0d6fd4fcb156e7ee03f2279ee","target":"record","created_at":"2026-07-05T06:31:07Z","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":"622629101353eac821c89285445a421d8d019cbe8c5757853f5e471673c5694f","cross_cats_sorted":["hep-th"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"gr-qc","submitted_at":"2022-12-20T18:04:17Z","title_canon_sha256":"def272b50908fce615fe6a6ee902398de2088b2b92452231e092cb3dfa7ced14"},"schema_version":"1.0","source":{"id":"2212.10486","kind":"arxiv","version":1}},"canonical_sha256":"12cf9b784d8ff045c3e738f67b377cd4ad9958710f8cc2acbc0413b2dc5f4006","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"12cf9b784d8ff045c3e738f67b377cd4ad9958710f8cc2acbc0413b2dc5f4006","first_computed_at":"2026-07-05T06:31:07.724724Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T06:31:07.724724Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"GqB8RZyZaPjTRZOAsd/a1s0zlMrSuLnPbvvOa5NgZVdjKSmOQcxNRKv/1KHDCrWMZkhE1S1IqNR9R1y7apRTCw==","signature_status":"signed_v1","signed_at":"2026-07-05T06:31:07.725122Z","signed_message":"canonical_sha256_bytes"},"source_id":"2212.10486","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:b412a7f7e856dac27ff96c95cd6bda9dafea0ca0d6fd4fcb156e7ee03f2279ee","sha256:f56d718574153e00e495972a3527206e3d9dff11b642a771a3ef3317747e783f"],"state_sha256":"60eed3f3f9d3dc602d127afe44fd7712ceef30487792a5179f46693bcb43ba1a"}