{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2024:E6EGKSJJFD2MJJIAD6RNB3XYKP","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":"d8044a11afae65fa151dec2ea479517376d289b0bc280cde326ba04bbdfc3a87","cross_cats_sorted":["physics.hist-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-04-22T07:04:51Z","title_canon_sha256":"d8a783a972b6a231f2646ab11390c47c02e6a4ef1e15b8b0dac19830766d947b"},"schema_version":"1.0","source":{"id":"2404.13928","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2404.13928","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"arxiv_version","alias_value":"2404.13928v3","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2404.13928","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"pith_short_12","alias_value":"E6EGKSJJFD2M","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"pith_short_16","alias_value":"E6EGKSJJFD2MJJIA","created_at":"2026-07-05T08:30:32Z"},{"alias_kind":"pith_short_8","alias_value":"E6EGKSJJ","created_at":"2026-07-05T08:30:32Z"}],"graph_snapshots":[{"event_id":"sha256:2fe235fa030b88dbc481c71aa4e91bb38a962bcf413c6f7ecda5aa175d2763e2","target":"graph","created_at":"2026-07-05T08:30:32Z","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/2404.13928/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"In previous work with Ken Wharton, it was proposed that Bell correlations are a special sort of selection artefact, explained by a combination of (i) collider bias and (ii) a boundary constraint on the collider variable. This requires no direct causal influence outside lightcones, and may hence offer a new way to reconcile Bell nonlocality and relativity. This piece outlines a new argument for the proposal. It explains how it is valid for a special class of ('W-shaped') Bell experiments involving delayed-choice entanglement swapping, and argues that it can be extended to the general ('V-shaped","authors_text":"Huw Price","cross_cats":["physics.hist-ph"],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-04-22T07:04:51Z","title":"W as the Edge of a Wedge: Bell Correlations via Constrained Colliders"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2404.13928","kind":"arxiv","version":3},"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":"sha256:8e58a436347fd442e3c9c14e20ca2ad98be9e0a8953a9eb1326da639e969da02","target":"record","created_at":"2026-07-05T08:30:32Z","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":"d8044a11afae65fa151dec2ea479517376d289b0bc280cde326ba04bbdfc3a87","cross_cats_sorted":["physics.hist-ph"],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2024-04-22T07:04:51Z","title_canon_sha256":"d8a783a972b6a231f2646ab11390c47c02e6a4ef1e15b8b0dac19830766d947b"},"schema_version":"1.0","source":{"id":"2404.13928","kind":"arxiv","version":3}},"canonical_sha256":"278865492928f4c4a5001fa2d0eef853df458e533a38166ebb206409a225bd8f","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"278865492928f4c4a5001fa2d0eef853df458e533a38166ebb206409a225bd8f","first_computed_at":"2026-07-05T08:30:32.975430Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T08:30:32.975430Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"k1VK3g4lNlUq8RS+MGCCOV6onuPVdAgLTYvJ3tbMoGjrszHyNmdJuV8wYDTBWDrmKmm3CUVimjJ+7EQxD/6OAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T08:30:32.975988Z","signed_message":"canonical_sha256_bytes"},"source_id":"2404.13928","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:8e58a436347fd442e3c9c14e20ca2ad98be9e0a8953a9eb1326da639e969da02","sha256:2fe235fa030b88dbc481c71aa4e91bb38a962bcf413c6f7ecda5aa175d2763e2"],"state_sha256":"3e5a8599afd48d609d05b593ed1b8874117021b05b41fe85ed0f1879a5b522c1"}