{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:KWLDTWPSP47GHCYDJCP2CHR43H","short_pith_number":"pith:KWLDTWPS","canonical_record":{"source":{"id":"1412.3942","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-12-12T10:33:09Z","cross_cats_sorted":[],"title_canon_sha256":"0a2f234d71885b3b9eb08116b860d11e8f6852dd2cbb626dab33fdc98014ce43","abstract_canon_sha256":"b2588f775df5c7bf0bb1c953a2775e7c0dda2720a72a34e5a9cfe3c5a440fb9b"},"schema_version":"1.0"},"canonical_sha256":"559639d9f27f3e638b03489fa11e3cd9e6ea9853969065ad992beea9e16b4e7a","source":{"kind":"arxiv","id":"1412.3942","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.3942","created_at":"2026-05-18T00:12:41Z"},{"alias_kind":"arxiv_version","alias_value":"1412.3942v1","created_at":"2026-05-18T00:12:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3942","created_at":"2026-05-18T00:12:41Z"},{"alias_kind":"pith_short_12","alias_value":"KWLDTWPSP47G","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_16","alias_value":"KWLDTWPSP47GHCYD","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_8","alias_value":"KWLDTWPS","created_at":"2026-05-18T12:28:35Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:KWLDTWPSP47GHCYDJCP2CHR43H","target":"record","payload":{"canonical_record":{"source":{"id":"1412.3942","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-12-12T10:33:09Z","cross_cats_sorted":[],"title_canon_sha256":"0a2f234d71885b3b9eb08116b860d11e8f6852dd2cbb626dab33fdc98014ce43","abstract_canon_sha256":"b2588f775df5c7bf0bb1c953a2775e7c0dda2720a72a34e5a9cfe3c5a440fb9b"},"schema_version":"1.0"},"canonical_sha256":"559639d9f27f3e638b03489fa11e3cd9e6ea9853969065ad992beea9e16b4e7a","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:12:41.082000Z","signature_b64":"EXp8MSzeuBnKJ0guQr/Tfj6chid7hxZEzei6606vrSeqUVFICK9ncYtBbkEgA+lvgtPAXxh0aUqlvoeKCdPvBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"559639d9f27f3e638b03489fa11e3cd9e6ea9853969065ad992beea9e16b4e7a","last_reissued_at":"2026-05-18T00:12:41.081469Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:12:41.081469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1412.3942","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":"2026-05-18T00:12:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"L7vLeFfcYiOXsN+ORYG/ckaHMJFKQLcyVKJG0Z7zK7USTAcMexIBSwLLLc68KfXnoD5Ps7PiznsHGWvBdYlkDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T12:06:19.070305Z"},"content_sha256":"974e42d1bc1e523acbd679803477457c3b6106645bcc1021f187929db2dfb03f","schema_version":"1.0","event_id":"sha256:974e42d1bc1e523acbd679803477457c3b6106645bcc1021f187929db2dfb03f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:KWLDTWPSP47GHCYDJCP2CHR43H","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Average Lorentz Self-Force From Electric Field Lines","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"physics.class-ph","authors_text":"Asrarul Haque, Sandeep Aashish","submitted_at":"2014-12-12T10:33:09Z","abstract_excerpt":"We generalize the derivation of electromagnetic fields of a charged particle moving with a constant acceleration [1] to a variable acceleration (piecewise constants) over a small finite time interval using Coulomb's law, relativistic transformations of electromagnetic fields and Thomson's construction [2]. We derive the average Lorentz self-force for a charged particle in arbitrary non-relativistic motion via averaging the fields at retarded time."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3942","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":"2026-05-18T00:12:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kaXVQ3l9ATNihcnctEFRpayjWiEorMYpDF/hQyp0lbhIcjzDKy/t/NFjoAq3c4mhYUuJJ49T8zz/Gll0+2LuAQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-01T12:06:19.070667Z"},"content_sha256":"1dd1b751b2502764153a55ec5950a1e6b8804e22661c3e6185c0f006f6a79400","schema_version":"1.0","event_id":"sha256:1dd1b751b2502764153a55ec5950a1e6b8804e22661c3e6185c0f006f6a79400"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/KWLDTWPSP47GHCYDJCP2CHR43H/bundle.json","state_url":"https://pith.science/pith/KWLDTWPSP47GHCYDJCP2CHR43H/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/KWLDTWPSP47GHCYDJCP2CHR43H/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":"2026-06-01T12:06:19Z","links":{"resolver":"https://pith.science/pith/KWLDTWPSP47GHCYDJCP2CHR43H","bundle":"https://pith.science/pith/KWLDTWPSP47GHCYDJCP2CHR43H/bundle.json","state":"https://pith.science/pith/KWLDTWPSP47GHCYDJCP2CHR43H/state.json","well_known_bundle":"https://pith.science/.well-known/pith/KWLDTWPSP47GHCYDJCP2CHR43H/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:KWLDTWPSP47GHCYDJCP2CHR43H","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":"b2588f775df5c7bf0bb1c953a2775e7c0dda2720a72a34e5a9cfe3c5a440fb9b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-12-12T10:33:09Z","title_canon_sha256":"0a2f234d71885b3b9eb08116b860d11e8f6852dd2cbb626dab33fdc98014ce43"},"schema_version":"1.0","source":{"id":"1412.3942","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1412.3942","created_at":"2026-05-18T00:12:41Z"},{"alias_kind":"arxiv_version","alias_value":"1412.3942v1","created_at":"2026-05-18T00:12:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1412.3942","created_at":"2026-05-18T00:12:41Z"},{"alias_kind":"pith_short_12","alias_value":"KWLDTWPSP47G","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_16","alias_value":"KWLDTWPSP47GHCYD","created_at":"2026-05-18T12:28:35Z"},{"alias_kind":"pith_short_8","alias_value":"KWLDTWPS","created_at":"2026-05-18T12:28:35Z"}],"graph_snapshots":[{"event_id":"sha256:1dd1b751b2502764153a55ec5950a1e6b8804e22661c3e6185c0f006f6a79400","target":"graph","created_at":"2026-05-18T00:12:41Z","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 generalize the derivation of electromagnetic fields of a charged particle moving with a constant acceleration [1] to a variable acceleration (piecewise constants) over a small finite time interval using Coulomb's law, relativistic transformations of electromagnetic fields and Thomson's construction [2]. We derive the average Lorentz self-force for a charged particle in arbitrary non-relativistic motion via averaging the fields at retarded time.","authors_text":"Asrarul Haque, Sandeep Aashish","cross_cats":[],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-12-12T10:33:09Z","title":"Average Lorentz Self-Force From Electric Field Lines"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1412.3942","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":"sha256:974e42d1bc1e523acbd679803477457c3b6106645bcc1021f187929db2dfb03f","target":"record","created_at":"2026-05-18T00:12:41Z","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":"b2588f775df5c7bf0bb1c953a2775e7c0dda2720a72a34e5a9cfe3c5a440fb9b","cross_cats_sorted":[],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-12-12T10:33:09Z","title_canon_sha256":"0a2f234d71885b3b9eb08116b860d11e8f6852dd2cbb626dab33fdc98014ce43"},"schema_version":"1.0","source":{"id":"1412.3942","kind":"arxiv","version":1}},"canonical_sha256":"559639d9f27f3e638b03489fa11e3cd9e6ea9853969065ad992beea9e16b4e7a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"559639d9f27f3e638b03489fa11e3cd9e6ea9853969065ad992beea9e16b4e7a","first_computed_at":"2026-05-18T00:12:41.081469Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:12:41.081469Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"EXp8MSzeuBnKJ0guQr/Tfj6chid7hxZEzei6606vrSeqUVFICK9ncYtBbkEgA+lvgtPAXxh0aUqlvoeKCdPvBQ==","signature_status":"signed_v1","signed_at":"2026-05-18T00:12:41.082000Z","signed_message":"canonical_sha256_bytes"},"source_id":"1412.3942","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:974e42d1bc1e523acbd679803477457c3b6106645bcc1021f187929db2dfb03f","sha256:1dd1b751b2502764153a55ec5950a1e6b8804e22661c3e6185c0f006f6a79400"],"state_sha256":"9890694c2e8602617f2c6e66680f57b5dc87412d26892d2cd24c1bbdf4ca2fcb"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"I/fS9sKOQVLmNguqMZYj2d43Uu+6UOvMfdRgQSagmAubSQlwalI1OjhMwcBYbz2HMC31Dt0PIJf+9liLzAUUCg==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-01T12:06:19.072542Z","bundle_sha256":"574807b4b1ce7f0e4dfbbbb3a24d4e3ba94d6edb3cb895f67d44c9b3271765b5"}}