{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:M3HBE5OH7KU3LM2CASINM33HZS","short_pith_number":"pith:M3HBE5OH","schema_version":"1.0","canonical_sha256":"66ce1275c7faa9b5b3420490d66f67cc941b193c6c6c69664b6a1dc090f3e60b","source":{"kind":"arxiv","id":"1202.6289","version":1},"attestation_state":"computed","paper":{"title":"Comment on \"Finite Size Corrections to the Radiation Reaction Force in Classical Electrodynamics\" [arXiv:1005.2617]","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"gr-qc","authors_text":"P. Forg\\'acs, P. Kov\\'acs, T. Herpay","submitted_at":"2012-02-28T17:10:38Z","abstract_excerpt":"In [1, arXiv:1005.2617] effective field theory methods have been employed to compute the equations of motion of a spherically symmetric charged shell of radius R, taking into account the radiation reaction force exerted by the shell's own electromagnetic field up to O(R^2). The authors of Ref. [1] have stated that the known result for the self force of the shell as can be found from Eq. (16.28) of the textbook of Jackson [2] (see also Chap. 4 in the review of Pearle [3]) is incorrect, in that the term linear in R should be absent. We claim that this conclusion of Ref. [1] is incorrect, and tha"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"1202.6289","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"gr-qc","submitted_at":"2012-02-28T17:10:38Z","cross_cats_sorted":["hep-ph","hep-th"],"title_canon_sha256":"290bb0d4d6d319c4d4852d587b536893edcc343fedd1fea7723595e9a7372232","abstract_canon_sha256":"841a92817e1484901ca290a530f6e36d7c062a3967f34e047ea1eafc9bae5b74"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:58:18.678597Z","signature_b64":"pSZ3yAjxLMxc/7TpNn7ehPh0jvzFuYk6L8iIHZtxJ0QQiJNH+nhyIqgHZdtW9IPLFQpJvnXjuGIFmcgmF18mDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"66ce1275c7faa9b5b3420490d66f67cc941b193c6c6c69664b6a1dc090f3e60b","last_reissued_at":"2026-05-18T01:58:18.678031Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:58:18.678031Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Comment on \"Finite Size Corrections to the Radiation Reaction Force in Classical Electrodynamics\" [arXiv:1005.2617]","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th"],"primary_cat":"gr-qc","authors_text":"P. Forg\\'acs, P. Kov\\'acs, T. Herpay","submitted_at":"2012-02-28T17:10:38Z","abstract_excerpt":"In [1, arXiv:1005.2617] effective field theory methods have been employed to compute the equations of motion of a spherically symmetric charged shell of radius R, taking into account the radiation reaction force exerted by the shell's own electromagnetic field up to O(R^2). The authors of Ref. [1] have stated that the known result for the self force of the shell as can be found from Eq. (16.28) of the textbook of Jackson [2] (see also Chap. 4 in the review of Pearle [3]) is incorrect, in that the term linear in R should be absent. We claim that this conclusion of Ref. [1] is incorrect, and tha"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1202.6289","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"},"aliases":[{"alias_kind":"arxiv","alias_value":"1202.6289","created_at":"2026-05-18T01:58:18.678105+00:00"},{"alias_kind":"arxiv_version","alias_value":"1202.6289v1","created_at":"2026-05-18T01:58:18.678105+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1202.6289","created_at":"2026-05-18T01:58:18.678105+00:00"},{"alias_kind":"pith_short_12","alias_value":"M3HBE5OH7KU3","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_16","alias_value":"M3HBE5OH7KU3LM2C","created_at":"2026-05-18T12:27:14.488303+00:00"},{"alias_kind":"pith_short_8","alias_value":"M3HBE5OH","created_at":"2026-05-18T12:27:14.488303+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS","json":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS.json","graph_json":"https://pith.science/api/pith-number/M3HBE5OH7KU3LM2CASINM33HZS/graph.json","events_json":"https://pith.science/api/pith-number/M3HBE5OH7KU3LM2CASINM33HZS/events.json","paper":"https://pith.science/paper/M3HBE5OH"},"agent_actions":{"view_html":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS","download_json":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS.json","view_paper":"https://pith.science/paper/M3HBE5OH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1202.6289&json=true","fetch_graph":"https://pith.science/api/pith-number/M3HBE5OH7KU3LM2CASINM33HZS/graph.json","fetch_events":"https://pith.science/api/pith-number/M3HBE5OH7KU3LM2CASINM33HZS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS/action/storage_attestation","attest_author":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS/action/author_attestation","sign_citation":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS/action/citation_signature","submit_replication":"https://pith.science/pith/M3HBE5OH7KU3LM2CASINM33HZS/action/replication_record"}},"created_at":"2026-05-18T01:58:18.678105+00:00","updated_at":"2026-05-18T01:58:18.678105+00:00"}