{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2004:VCOUZC23WSD362QM6PSAE6HNCN","short_pith_number":"pith:VCOUZC23","canonical_record":{"source":{"id":"quant-ph/0407162","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"quant-ph","submitted_at":"2004-07-20T16:50:08Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b02e805a89b1817da22684ddfc40c99985f3d0825373f4701253dd4ef108892c","abstract_canon_sha256":"71de99cf6ec11c86e34f7aa15e3357dbe0bda54d2777228ebf972b10eee3f716"},"schema_version":"1.0"},"canonical_sha256":"a89d4c8b5bb487bf6a0cf3e40278ed1346c0471d95a45486186502b35dbcadd5","source":{"kind":"arxiv","id":"quant-ph/0407162","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"quant-ph/0407162","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"arxiv_version","alias_value":"quant-ph/0407162v1","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.quant-ph/0407162","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"pith_short_12","alias_value":"VCOUZC23WSD3","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"pith_short_16","alias_value":"VCOUZC23WSD362QM","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"pith_short_8","alias_value":"VCOUZC23","created_at":"2026-07-04T15:23:29Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2004:VCOUZC23WSD362QM6PSAE6HNCN","target":"record","payload":{"canonical_record":{"source":{"id":"quant-ph/0407162","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"quant-ph","submitted_at":"2004-07-20T16:50:08Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"b02e805a89b1817da22684ddfc40c99985f3d0825373f4701253dd4ef108892c","abstract_canon_sha256":"71de99cf6ec11c86e34f7aa15e3357dbe0bda54d2777228ebf972b10eee3f716"},"schema_version":"1.0"},"canonical_sha256":"a89d4c8b5bb487bf6a0cf3e40278ed1346c0471d95a45486186502b35dbcadd5","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:23:29.929371Z","signature_b64":"WywmRp01SEK9cRscMxytWruB+zanxVX28Rb1mSLvfDr1QT4QZIZcx3N8z0Y28z8U+sC7L0sSCTmmN94bKW+GCw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a89d4c8b5bb487bf6a0cf3e40278ed1346c0471d95a45486186502b35dbcadd5","last_reissued_at":"2026-07-04T15:23:29.928953Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:23:29.928953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"quant-ph/0407162","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":"2026-07-04T15:23:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"vAut3C9PwAuyeQ9cYCmPIFZppfXL7xWOwJXPlG5IJ8TAo9/qM247yZdyyOI6LYb4hG6nNk/+1ok6m9EkXFS/Bg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-02T22:40:24.925823Z"},"content_sha256":"e873b6d88d6b03a4a5063f7d7c375ebcc71d97f67b8953390345a941a0acb6b3","schema_version":"1.0","event_id":"sha256:e873b6d88d6b03a4a5063f7d7c375ebcc71d97f67b8953390345a941a0acb6b3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2004:VCOUZC23WSD362QM6PSAE6HNCN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"The Lorentz-Dirac force from QED for linear acceleration","license":"","headline":"","cross_cats":["hep-th"],"primary_cat":"quant-ph","authors_text":"Atsushi Higuchi, Giles D. R. Martin (Univ. of York)","submitted_at":"2004-07-20T16:50:08Z","abstract_excerpt":"We investigate the motion of a wave packet of a charged scalar particle linearly accelerated by a static potential in quantum electrodynamics. We calculate the expectation value of the position of the charged particle after the acceleration to first order in the fine structure constant in the hbar -> 0 limit. We find that the change in the expectation value of the position (the position shift) due to radiation reaction agrees exactly with the result obtained using the Lorentz-Dirac force in classical electrodynamics. We also point out that the one-loop correction to the potential may contribut"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"quant-ph/0407162","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/quant-ph/0407162/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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":"2026-07-04T15:23:29Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"bseU+tm8D3RJzZf7Eshtn3GhqlOMhhZ/OOCzhp7XKZD/U3W6aSSAWhDdsVozn/vqmdz8aA3rhn/G4xNKWr7CCg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-08-02T22:40:24.926699Z"},"content_sha256":"fc6d53dd5ee7452bb6cb58f2bed961a2cc41b935e66a707ce2b0d6df261a7b56","schema_version":"1.0","event_id":"sha256:fc6d53dd5ee7452bb6cb58f2bed961a2cc41b935e66a707ce2b0d6df261a7b56"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/VCOUZC23WSD362QM6PSAE6HNCN/bundle.json","state_url":"https://pith.science/pith/VCOUZC23WSD362QM6PSAE6HNCN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/VCOUZC23WSD362QM6PSAE6HNCN/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":"2026-08-02T22:40:24Z","links":{"resolver":"https://pith.science/pith/VCOUZC23WSD362QM6PSAE6HNCN","bundle":"https://pith.science/pith/VCOUZC23WSD362QM6PSAE6HNCN/bundle.json","state":"https://pith.science/pith/VCOUZC23WSD362QM6PSAE6HNCN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/VCOUZC23WSD362QM6PSAE6HNCN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2004:VCOUZC23WSD362QM6PSAE6HNCN","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":"71de99cf6ec11c86e34f7aa15e3357dbe0bda54d2777228ebf972b10eee3f716","cross_cats_sorted":["hep-th"],"license":"","primary_cat":"quant-ph","submitted_at":"2004-07-20T16:50:08Z","title_canon_sha256":"b02e805a89b1817da22684ddfc40c99985f3d0825373f4701253dd4ef108892c"},"schema_version":"1.0","source":{"id":"quant-ph/0407162","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"quant-ph/0407162","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"arxiv_version","alias_value":"quant-ph/0407162v1","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.quant-ph/0407162","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"pith_short_12","alias_value":"VCOUZC23WSD3","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"pith_short_16","alias_value":"VCOUZC23WSD362QM","created_at":"2026-07-04T15:23:29Z"},{"alias_kind":"pith_short_8","alias_value":"VCOUZC23","created_at":"2026-07-04T15:23:29Z"}],"graph_snapshots":[{"event_id":"sha256:fc6d53dd5ee7452bb6cb58f2bed961a2cc41b935e66a707ce2b0d6df261a7b56","target":"graph","created_at":"2026-07-04T15:23:29Z","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/quant-ph/0407162/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the motion of a wave packet of a charged scalar particle linearly accelerated by a static potential in quantum electrodynamics. We calculate the expectation value of the position of the charged particle after the acceleration to first order in the fine structure constant in the hbar -> 0 limit. We find that the change in the expectation value of the position (the position shift) due to radiation reaction agrees exactly with the result obtained using the Lorentz-Dirac force in classical electrodynamics. We also point out that the one-loop correction to the potential may contribut","authors_text":"Atsushi Higuchi, Giles D. R. Martin (Univ. of York)","cross_cats":["hep-th"],"headline":"","license":"","primary_cat":"quant-ph","submitted_at":"2004-07-20T16:50:08Z","title":"The Lorentz-Dirac force from QED for linear acceleration"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"quant-ph/0407162","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:e873b6d88d6b03a4a5063f7d7c375ebcc71d97f67b8953390345a941a0acb6b3","target":"record","created_at":"2026-07-04T15:23:29Z","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":"71de99cf6ec11c86e34f7aa15e3357dbe0bda54d2777228ebf972b10eee3f716","cross_cats_sorted":["hep-th"],"license":"","primary_cat":"quant-ph","submitted_at":"2004-07-20T16:50:08Z","title_canon_sha256":"b02e805a89b1817da22684ddfc40c99985f3d0825373f4701253dd4ef108892c"},"schema_version":"1.0","source":{"id":"quant-ph/0407162","kind":"arxiv","version":1}},"canonical_sha256":"a89d4c8b5bb487bf6a0cf3e40278ed1346c0471d95a45486186502b35dbcadd5","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"a89d4c8b5bb487bf6a0cf3e40278ed1346c0471d95a45486186502b35dbcadd5","first_computed_at":"2026-07-04T15:23:29.928953Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-04T15:23:29.928953Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"WywmRp01SEK9cRscMxytWruB+zanxVX28Rb1mSLvfDr1QT4QZIZcx3N8z0Y28z8U+sC7L0sSCTmmN94bKW+GCw==","signature_status":"signed_v1","signed_at":"2026-07-04T15:23:29.929371Z","signed_message":"canonical_sha256_bytes"},"source_id":"quant-ph/0407162","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:e873b6d88d6b03a4a5063f7d7c375ebcc71d97f67b8953390345a941a0acb6b3","sha256:fc6d53dd5ee7452bb6cb58f2bed961a2cc41b935e66a707ce2b0d6df261a7b56"],"state_sha256":"5d0381c81f1660fe2d525731380315885d0f9683322a2baeb2a85578aa4e9b7c"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"sASld4ZcFlchkRG+/SPqyU6PopLDzDfpG7FizzGrVqJuD0Tou4VJPA+Yx/9s2WF97PyxH0GdzZyVEw2BJKHlDQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-08-02T22:40:24.933915Z","bundle_sha256":"f64dc8858c9525e6082567eba65a22008edd3709fba1e0145d5ef646ddb3a0dd"}}