{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2011:WHAQNQC27DXPCOYBJLL3RZKTH5","short_pith_number":"pith:WHAQNQC2","canonical_record":{"source":{"id":"1112.2665","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-12-12T19:29:27Z","cross_cats_sorted":["physics.comp-ph","physics.optics"],"title_canon_sha256":"8fed9c337b5854509d5158e8870153291e5f4959c71bbdc109aca29a6de18783","abstract_canon_sha256":"cf2567406dbc91a59db9def8d0f7a5440b1ac3ec153e698d928381f0e1fc96d0"},"schema_version":"1.0"},"canonical_sha256":"b1c106c05af8eef13b014ad7b8e5533f7abf583de9942bd6c896d34019e3ec86","source":{"kind":"arxiv","id":"1112.2665","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.2665","created_at":"2026-05-18T04:06:33Z"},{"alias_kind":"arxiv_version","alias_value":"1112.2665v1","created_at":"2026-05-18T04:06:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.2665","created_at":"2026-05-18T04:06:33Z"},{"alias_kind":"pith_short_12","alias_value":"WHAQNQC27DXP","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WHAQNQC27DXPCOYB","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WHAQNQC2","created_at":"2026-05-18T12:26:44Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2011:WHAQNQC27DXPCOYBJLL3RZKTH5","target":"record","payload":{"canonical_record":{"source":{"id":"1112.2665","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-12-12T19:29:27Z","cross_cats_sorted":["physics.comp-ph","physics.optics"],"title_canon_sha256":"8fed9c337b5854509d5158e8870153291e5f4959c71bbdc109aca29a6de18783","abstract_canon_sha256":"cf2567406dbc91a59db9def8d0f7a5440b1ac3ec153e698d928381f0e1fc96d0"},"schema_version":"1.0"},"canonical_sha256":"b1c106c05af8eef13b014ad7b8e5533f7abf583de9942bd6c896d34019e3ec86","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:06:33.668075Z","signature_b64":"dBVCKSvMQ71SoEihRBM+iSt54F3vsH1RTduwaXTFDfCYwmGhNogLZO8bIOuBV7DybXJXlxbnMT6dPZrb95ziAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b1c106c05af8eef13b014ad7b8e5533f7abf583de9942bd6c896d34019e3ec86","last_reissued_at":"2026-05-18T04:06:33.667271Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:06:33.667271Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1112.2665","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":"2026-05-18T04:06:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kd5jBjyEpr24kdE/T9XwPIr2Sgg3RtAnE5Wi3Jxp15O43dkAVUlSyyFGDT4S/5oX8fxI1qOWjdZ4/5ocFTBMBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T03:00:35.433085Z"},"content_sha256":"87525ce8b318045920b795819c204bca4c0112811b0aca3a7a93fafcbb6620b3","schema_version":"1.0","event_id":"sha256:87525ce8b318045920b795819c204bca4c0112811b0aca3a7a93fafcbb6620b3"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2011:WHAQNQC27DXPCOYBJLL3RZKTH5","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Analysis of multipath interference in three-slit experiments","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["physics.comp-ph","physics.optics"],"primary_cat":"quant-ph","authors_text":"H. De Raedt, K. Hess, K. Michielsen","submitted_at":"2011-12-12T19:29:27Z","abstract_excerpt":"It is demonstrated that the three-slit interference, as obtained from explicit solutions of Maxwell's equations for realistic models of three-slit devices, including an idealized version of the three-slit device used in a recent three-slit experiment with light (U. Sinha {\\sl et al.}, Science 329, 418 (2010)), is nonzero. The hypothesis that the three-slit interference should be zero is the result of dropping the one-to-one correspondence between the symbols in the mathematical theory and the different experimental configurations, opening the route to conclusions that cannot be derived from th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.2665","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":"2026-05-18T04:06:33Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"YbgK1Hodx6vKhpLmFCizYbF8f8cR1HZlQWgOHyWoa2j57Xoflx6rYCFOs+p8kz0ACLIcBzuA2rW2g+gfb3XZCA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-23T03:00:35.433763Z"},"content_sha256":"3e80754515a21740b596aa62b7b0effd5ee7a8b1533e90e49cca2d53901b3df0","schema_version":"1.0","event_id":"sha256:3e80754515a21740b596aa62b7b0effd5ee7a8b1533e90e49cca2d53901b3df0"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/WHAQNQC27DXPCOYBJLL3RZKTH5/bundle.json","state_url":"https://pith.science/pith/WHAQNQC27DXPCOYBJLL3RZKTH5/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/WHAQNQC27DXPCOYBJLL3RZKTH5/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":"2026-05-23T03:00:35Z","links":{"resolver":"https://pith.science/pith/WHAQNQC27DXPCOYBJLL3RZKTH5","bundle":"https://pith.science/pith/WHAQNQC27DXPCOYBJLL3RZKTH5/bundle.json","state":"https://pith.science/pith/WHAQNQC27DXPCOYBJLL3RZKTH5/state.json","well_known_bundle":"https://pith.science/.well-known/pith/WHAQNQC27DXPCOYBJLL3RZKTH5/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2011:WHAQNQC27DXPCOYBJLL3RZKTH5","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":"cf2567406dbc91a59db9def8d0f7a5440b1ac3ec153e698d928381f0e1fc96d0","cross_cats_sorted":["physics.comp-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-12-12T19:29:27Z","title_canon_sha256":"8fed9c337b5854509d5158e8870153291e5f4959c71bbdc109aca29a6de18783"},"schema_version":"1.0","source":{"id":"1112.2665","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1112.2665","created_at":"2026-05-18T04:06:33Z"},{"alias_kind":"arxiv_version","alias_value":"1112.2665v1","created_at":"2026-05-18T04:06:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1112.2665","created_at":"2026-05-18T04:06:33Z"},{"alias_kind":"pith_short_12","alias_value":"WHAQNQC27DXP","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_16","alias_value":"WHAQNQC27DXPCOYB","created_at":"2026-05-18T12:26:44Z"},{"alias_kind":"pith_short_8","alias_value":"WHAQNQC2","created_at":"2026-05-18T12:26:44Z"}],"graph_snapshots":[{"event_id":"sha256:3e80754515a21740b596aa62b7b0effd5ee7a8b1533e90e49cca2d53901b3df0","target":"graph","created_at":"2026-05-18T04:06:33Z","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":"It is demonstrated that the three-slit interference, as obtained from explicit solutions of Maxwell's equations for realistic models of three-slit devices, including an idealized version of the three-slit device used in a recent three-slit experiment with light (U. Sinha {\\sl et al.}, Science 329, 418 (2010)), is nonzero. The hypothesis that the three-slit interference should be zero is the result of dropping the one-to-one correspondence between the symbols in the mathematical theory and the different experimental configurations, opening the route to conclusions that cannot be derived from th","authors_text":"H. De Raedt, K. Hess, K. Michielsen","cross_cats":["physics.comp-ph","physics.optics"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-12-12T19:29:27Z","title":"Analysis of multipath interference in three-slit experiments"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1112.2665","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":"sha256:87525ce8b318045920b795819c204bca4c0112811b0aca3a7a93fafcbb6620b3","target":"record","created_at":"2026-05-18T04:06:33Z","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":"cf2567406dbc91a59db9def8d0f7a5440b1ac3ec153e698d928381f0e1fc96d0","cross_cats_sorted":["physics.comp-ph","physics.optics"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2011-12-12T19:29:27Z","title_canon_sha256":"8fed9c337b5854509d5158e8870153291e5f4959c71bbdc109aca29a6de18783"},"schema_version":"1.0","source":{"id":"1112.2665","kind":"arxiv","version":1}},"canonical_sha256":"b1c106c05af8eef13b014ad7b8e5533f7abf583de9942bd6c896d34019e3ec86","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"b1c106c05af8eef13b014ad7b8e5533f7abf583de9942bd6c896d34019e3ec86","first_computed_at":"2026-05-18T04:06:33.667271Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T04:06:33.667271Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"dBVCKSvMQ71SoEihRBM+iSt54F3vsH1RTduwaXTFDfCYwmGhNogLZO8bIOuBV7DybXJXlxbnMT6dPZrb95ziAA==","signature_status":"signed_v1","signed_at":"2026-05-18T04:06:33.668075Z","signed_message":"canonical_sha256_bytes"},"source_id":"1112.2665","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:87525ce8b318045920b795819c204bca4c0112811b0aca3a7a93fafcbb6620b3","sha256:3e80754515a21740b596aa62b7b0effd5ee7a8b1533e90e49cca2d53901b3df0"],"state_sha256":"8b8f83fbd0d5f039d7c88d61803bd7c15ac5365fa04de75a99f466f303c1b765"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"5LWaFD/HJLsuc+cBEm3lDbIimJ1dVoDhOC+ymwgWP7MZ9y7Jbaq2TPOXDxbgeUYT8oLOguB1J1VgSNxeeXNmDw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-23T03:00:35.437252Z","bundle_sha256":"9958cb488ded3f3acf4accf9c3fe13ec757d3fc6bcc67fa379337dafa8d3d2a4"}}