{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:4V2FG5QCV7GXUHEA5GJAUUO624","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":"7baa11ac7eb0d90b7d6ee44e675047417b34e829f0b9d83b90827259567e4dda","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2025-10-18T03:33:25Z","title_canon_sha256":"0690207006319fd6f5db45216aa85cc0fc5873f280c8ad4724638370fd3bc3da"},"schema_version":"1.0","source":{"id":"2510.16329","kind":"arxiv","version":4}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2510.16329","created_at":"2026-06-04T01:08:33Z"},{"alias_kind":"arxiv_version","alias_value":"2510.16329v4","created_at":"2026-06-04T01:08:33Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2510.16329","created_at":"2026-06-04T01:08:33Z"},{"alias_kind":"pith_short_12","alias_value":"4V2FG5QCV7GX","created_at":"2026-06-04T01:08:33Z"},{"alias_kind":"pith_short_16","alias_value":"4V2FG5QCV7GXUHEA","created_at":"2026-06-04T01:08:33Z"},{"alias_kind":"pith_short_8","alias_value":"4V2FG5QC","created_at":"2026-06-04T01:08:33Z"}],"graph_snapshots":[{"event_id":"sha256:eb5dd10e9ae79ebdcf7f733f33e9c7b7b5d7e800530a40d0668a7dc3fe42a7b0","target":"graph","created_at":"2026-06-04T01:08:33Z","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":4,"items":[{"attestation":"unclaimed","claim_id":"C1","kind":"strongest_claim","source":"verdict.strongest_claim","status":"machine_extracted","text":"the observed diffraction pattern arises from projection of the photon state onto a single bright mode by identifying the detectable and undetectable modes, with photons detected at intensity minima having zero probability, as they reside in modes spanning an infinite-dimensional dark subspace."},{"attestation":"unclaimed","claim_id":"C2","kind":"weakest_assumption","source":"verdict.weakest_assumption","status":"machine_extracted","text":"That the bright/dark distinction introduced for a finite number of discrete paths in the cited PRL paper extends without additional postulates to a complete, orthonormal, detector-oriented basis for the continuous-mode single-slit case (abstract and §2–3)."},{"attestation":"unclaimed","claim_id":"C3","kind":"one_line_summary","source":"verdict.one_line_summary","status":"machine_extracted","text":"Diffraction arises when photons project onto one bright mode in an infinite-dimensional detector basis while all intensity minima lie in an undetectable dark subspace."},{"attestation":"unclaimed","claim_id":"C4","kind":"headline","source":"verdict.pith_extraction.headline","status":"machine_extracted","text":"Diffraction patterns arise because photons project onto one bright mode while occupying an infinite dark subspace at minima."}],"snapshot_sha256":"6c31f38961fc2fa3e39f09d0fb19dfabd1212315d8c93466e0654ddf1e98835e"},"formal_canon":{"evidence_count":2,"snapshot_sha256":"1f8ba4e4cd1ec8f467975c68753c0289c0175539399d1de1e260b9c26f23dd39"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2510.16329/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Building upon the recently introduced particle interpretation of the double-slit experiment [Phys. Rev. Lett. 134, 133603 (2025)] which attributes interference phenomena to detector-coupled (bright) and detector-uncoupled (dark) states of light, we develop a continuous-mode extension of the bright- and dark-state framework. This extension addresses a conceptual distinction between interference and diffraction, that is, the transition from a finite set of discrete paths to a continuum of modes. Through the construction of a complete detector-oriented basis for single-slit diffraction, we demons","authors_text":"Jian-Jian Cheng, Jun-Ling Che, Lin Zhang, Ming-Liang Hu","cross_cats":[],"headline":"Diffraction patterns arise because photons project onto one bright mode while occupying an infinite dark subspace at minima.","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2025-10-18T03:33:25Z","title":"Quantum Origin of Diffraction from Bright and Dark States"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2510.16329","kind":"arxiv","version":4},"verdict":{"created_at":"2026-05-18T06:50:58.135194Z","id":"52e2b5f9-feb7-41b5-96f6-fc7729834b38","model_set":{"reader":"grok-4.3"},"one_line_summary":"Diffraction arises when photons project onto one bright mode in an infinite-dimensional detector basis while all intensity minima lie in an undetectable dark subspace.","pipeline_version":"pith-pipeline@v0.9.0","pith_extraction_headline":"Diffraction patterns arise because photons project onto one bright mode while occupying an infinite dark subspace at minima.","strongest_claim":"the observed diffraction pattern arises from projection of the photon state onto a single bright mode by identifying the detectable and undetectable modes, with photons detected at intensity minima having zero probability, as they reside in modes spanning an infinite-dimensional dark subspace.","weakest_assumption":"That the bright/dark distinction introduced for a finite number of discrete paths in the cited PRL paper extends without additional postulates to a complete, orthonormal, detector-oriented basis for the continuous-mode single-slit case (abstract and §2–3)."}},"verdict_id":"52e2b5f9-feb7-41b5-96f6-fc7729834b38"}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:7c0e76827fd57aec9182359eeb3a787948c965fef6961e1d28484c0bef19baee","target":"record","created_at":"2026-06-04T01:08:33Z","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":"7baa11ac7eb0d90b7d6ee44e675047417b34e829f0b9d83b90827259567e4dda","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2025-10-18T03:33:25Z","title_canon_sha256":"0690207006319fd6f5db45216aa85cc0fc5873f280c8ad4724638370fd3bc3da"},"schema_version":"1.0","source":{"id":"2510.16329","kind":"arxiv","version":4}},"canonical_sha256":"e574537602afcd7a1c80e9920a51ded73cd3e2765fda58be711063b8fe9d016a","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"e574537602afcd7a1c80e9920a51ded73cd3e2765fda58be711063b8fe9d016a","first_computed_at":"2026-06-04T01:08:33.947727Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-04T01:08:33.947727Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BW7RhkjoMZ5JOQ1utkWYmV5i0x7RGvzyqZ7Cop1DMst7KTHaXQwATAPhe8yilhc8YodUzMRd/dn93k7aT/c4Dw==","signature_status":"signed_v1","signed_at":"2026-06-04T01:08:33.948443Z","signed_message":"canonical_sha256_bytes"},"source_id":"2510.16329","source_kind":"arxiv","source_version":4}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7c0e76827fd57aec9182359eeb3a787948c965fef6961e1d28484c0bef19baee","sha256:eb5dd10e9ae79ebdcf7f733f33e9c7b7b5d7e800530a40d0668a7dc3fe42a7b0"],"state_sha256":"392845d8957c878f81a590fe5e8ab73347e4a553148744e06742b45653046a41"}