{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2014:PX2LWAPQBHMIME2NSXXENOZIHN","short_pith_number":"pith:PX2LWAPQ","canonical_record":{"source":{"id":"1408.3745","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-08-16T16:34:46Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"14e2fd8cf6089c2f6e66f3d5503a4135ea22f86c34531f624f713f3ddbf68714","abstract_canon_sha256":"43a02db3699c084e33bfd67da6956e0833848a43e137a1855f306aa5a7148325"},"schema_version":"1.0"},"canonical_sha256":"7df4bb01f009d886134d95ee46bb283b43c2a3847c043fa313111ac46d9cf7f8","source":{"kind":"arxiv","id":"1408.3745","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.3745","created_at":"2026-05-18T02:44:16Z"},{"alias_kind":"arxiv_version","alias_value":"1408.3745v2","created_at":"2026-05-18T02:44:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.3745","created_at":"2026-05-18T02:44:16Z"},{"alias_kind":"pith_short_12","alias_value":"PX2LWAPQBHMI","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"PX2LWAPQBHMIME2N","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"PX2LWAPQ","created_at":"2026-05-18T12:28:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2014:PX2LWAPQBHMIME2NSXXENOZIHN","target":"record","payload":{"canonical_record":{"source":{"id":"1408.3745","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-08-16T16:34:46Z","cross_cats_sorted":["quant-ph"],"title_canon_sha256":"14e2fd8cf6089c2f6e66f3d5503a4135ea22f86c34531f624f713f3ddbf68714","abstract_canon_sha256":"43a02db3699c084e33bfd67da6956e0833848a43e137a1855f306aa5a7148325"},"schema_version":"1.0"},"canonical_sha256":"7df4bb01f009d886134d95ee46bb283b43c2a3847c043fa313111ac46d9cf7f8","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:44:16.065807Z","signature_b64":"5rpnotoBoKXyfHYwBzYQNgVDfuW/lRnPZDBMXBMBcIMO7yZ8y4+DN23/pPq3EKqzeGaM9OtoD8tzBe11RQhVDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7df4bb01f009d886134d95ee46bb283b43c2a3847c043fa313111ac46d9cf7f8","last_reissued_at":"2026-05-18T02:44:16.065234Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:44:16.065234Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1408.3745","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T02:44:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"PbwECEDZIddPptKG9kAPE4K1OE+ZnzKNdvXUABdRe0vHtYglKjntOkyWMunJa5WVVwZeRXfLeSadbsoWTKqlCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T20:55:54.722444Z"},"content_sha256":"839f797ade952f4f3f7134c8cfd01bdb9d607289052d230d38a41dd5ef0daac6","schema_version":"1.0","event_id":"sha256:839f797ade952f4f3f7134c8cfd01bdb9d607289052d230d38a41dd5ef0daac6"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2014:PX2LWAPQBHMIME2NSXXENOZIHN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Classical Interaction of a Magnet and a Point Charge: The Classical Electromagnetic Forces Responsible for the Aharonov-Bohm Phase Shift","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["quant-ph"],"primary_cat":"physics.class-ph","authors_text":"Timothy H. Boyer","submitted_at":"2014-08-16T16:34:46Z","abstract_excerpt":"A new classical electromagnetic analysis is presented suggesting that the Aharonov-Bohm phase shift is overwhelmingly likely to arise from a classical lag effect based upon classical electromagnetic forces. The analysis makes use of several aspects of classical electromagnetic theory which are unfamiliar to most physicists, including the Darwin Lagrangian, acceleration-based electric fields, internal electromagnetic momentum in a magnet, and a magnet model involving at least three mutually-interacting particles. Only when the acceleration-based electric forces acting on the passing charge are "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.3745","kind":"arxiv","version":2},"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":"2026-05-18T02:44:16Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"lWo5iIpSDGjdh88kSJss5EqMKl9N2sQkYs0LYKKVMabBmJt2Hysj5SdS3zoJxtconZVUYia+Rw27hJObTKoGBA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-06T20:55:54.723104Z"},"content_sha256":"4aeecec96f781f100d5b0861166e315ee5045499956221ddf0f2f4dc1b184950","schema_version":"1.0","event_id":"sha256:4aeecec96f781f100d5b0861166e315ee5045499956221ddf0f2f4dc1b184950"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/PX2LWAPQBHMIME2NSXXENOZIHN/bundle.json","state_url":"https://pith.science/pith/PX2LWAPQBHMIME2NSXXENOZIHN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/PX2LWAPQBHMIME2NSXXENOZIHN/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":"2026-06-06T20:55:54Z","links":{"resolver":"https://pith.science/pith/PX2LWAPQBHMIME2NSXXENOZIHN","bundle":"https://pith.science/pith/PX2LWAPQBHMIME2NSXXENOZIHN/bundle.json","state":"https://pith.science/pith/PX2LWAPQBHMIME2NSXXENOZIHN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/PX2LWAPQBHMIME2NSXXENOZIHN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2014:PX2LWAPQBHMIME2NSXXENOZIHN","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":"43a02db3699c084e33bfd67da6956e0833848a43e137a1855f306aa5a7148325","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-08-16T16:34:46Z","title_canon_sha256":"14e2fd8cf6089c2f6e66f3d5503a4135ea22f86c34531f624f713f3ddbf68714"},"schema_version":"1.0","source":{"id":"1408.3745","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1408.3745","created_at":"2026-05-18T02:44:16Z"},{"alias_kind":"arxiv_version","alias_value":"1408.3745v2","created_at":"2026-05-18T02:44:16Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.3745","created_at":"2026-05-18T02:44:16Z"},{"alias_kind":"pith_short_12","alias_value":"PX2LWAPQBHMI","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_16","alias_value":"PX2LWAPQBHMIME2N","created_at":"2026-05-18T12:28:43Z"},{"alias_kind":"pith_short_8","alias_value":"PX2LWAPQ","created_at":"2026-05-18T12:28:43Z"}],"graph_snapshots":[{"event_id":"sha256:4aeecec96f781f100d5b0861166e315ee5045499956221ddf0f2f4dc1b184950","target":"graph","created_at":"2026-05-18T02:44:16Z","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"},"paper":{"abstract_excerpt":"A new classical electromagnetic analysis is presented suggesting that the Aharonov-Bohm phase shift is overwhelmingly likely to arise from a classical lag effect based upon classical electromagnetic forces. The analysis makes use of several aspects of classical electromagnetic theory which are unfamiliar to most physicists, including the Darwin Lagrangian, acceleration-based electric fields, internal electromagnetic momentum in a magnet, and a magnet model involving at least three mutually-interacting particles. Only when the acceleration-based electric forces acting on the passing charge are ","authors_text":"Timothy H. Boyer","cross_cats":["quant-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-08-16T16:34:46Z","title":"Classical Interaction of a Magnet and a Point Charge: The Classical Electromagnetic Forces Responsible for the Aharonov-Bohm Phase Shift"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.3745","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":"sha256:839f797ade952f4f3f7134c8cfd01bdb9d607289052d230d38a41dd5ef0daac6","target":"record","created_at":"2026-05-18T02:44:16Z","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":"43a02db3699c084e33bfd67da6956e0833848a43e137a1855f306aa5a7148325","cross_cats_sorted":["quant-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"physics.class-ph","submitted_at":"2014-08-16T16:34:46Z","title_canon_sha256":"14e2fd8cf6089c2f6e66f3d5503a4135ea22f86c34531f624f713f3ddbf68714"},"schema_version":"1.0","source":{"id":"1408.3745","kind":"arxiv","version":2}},"canonical_sha256":"7df4bb01f009d886134d95ee46bb283b43c2a3847c043fa313111ac46d9cf7f8","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"7df4bb01f009d886134d95ee46bb283b43c2a3847c043fa313111ac46d9cf7f8","first_computed_at":"2026-05-18T02:44:16.065234Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T02:44:16.065234Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"5rpnotoBoKXyfHYwBzYQNgVDfuW/lRnPZDBMXBMBcIMO7yZ8y4+DN23/pPq3EKqzeGaM9OtoD8tzBe11RQhVDQ==","signature_status":"signed_v1","signed_at":"2026-05-18T02:44:16.065807Z","signed_message":"canonical_sha256_bytes"},"source_id":"1408.3745","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:839f797ade952f4f3f7134c8cfd01bdb9d607289052d230d38a41dd5ef0daac6","sha256:4aeecec96f781f100d5b0861166e315ee5045499956221ddf0f2f4dc1b184950"],"state_sha256":"04aae3075a66f648fc65f72f6916cf3174d886c440de09efc8e8cdfbb63c832d"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5+hpgrdJGg/u3sxGpSQebAdlJ5UWoKnZn1QHwOyLplQPqN64/1HY7Y2xJ/pAN0jirPVd8jEt6AkRr6Q1VLfFDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-06T20:55:54.726424Z","bundle_sha256":"c12abab94dee216b8d136d246f326c23ce41a91cef8fa01126785b7a54dc0ab8"}}