{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2003:O6SS3AELBN6W4VNMWVE7NG46VY","short_pith_number":"pith:O6SS3AEL","canonical_record":{"source":{"id":"quant-ph/0308038","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"quant-ph","submitted_at":"2003-08-06T17:33:19Z","cross_cats_sorted":[],"title_canon_sha256":"97c5c8e22221251f8b270a57d90e49bb68c6ddf50208a617c08f2be735af7665","abstract_canon_sha256":"dd5ec630761ba52efcdb29cb87f7ea76f4332f93377a93479a1cd4784fde6c5a"},"schema_version":"1.0"},"canonical_sha256":"77a52d808b0b7d6e55acb549f69b9eae082fad79db08f1fce9905373232e6aea","source":{"kind":"arxiv","id":"quant-ph/0308038","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"quant-ph/0308038","created_at":"2026-05-18T01:08:59Z"},{"alias_kind":"arxiv_version","alias_value":"quant-ph/0308038v2","created_at":"2026-05-18T01:08:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.quant-ph/0308038","created_at":"2026-05-18T01:08:59Z"},{"alias_kind":"pith_short_12","alias_value":"O6SS3AELBN6W","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"O6SS3AELBN6W4VNM","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"O6SS3AEL","created_at":"2026-05-18T12:25:52Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2003:O6SS3AELBN6W4VNMWVE7NG46VY","target":"record","payload":{"canonical_record":{"source":{"id":"quant-ph/0308038","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"quant-ph","submitted_at":"2003-08-06T17:33:19Z","cross_cats_sorted":[],"title_canon_sha256":"97c5c8e22221251f8b270a57d90e49bb68c6ddf50208a617c08f2be735af7665","abstract_canon_sha256":"dd5ec630761ba52efcdb29cb87f7ea76f4332f93377a93479a1cd4784fde6c5a"},"schema_version":"1.0"},"canonical_sha256":"77a52d808b0b7d6e55acb549f69b9eae082fad79db08f1fce9905373232e6aea","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:08:59.317203Z","signature_b64":"NED3bHUq0r0hZX6YfBu3iSA6/EmfQpGxAdRjutw4381Uojwn8ks0PB0VkdC9XWpBKPMfSRD0LykZ4uWdhhcvBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"77a52d808b0b7d6e55acb549f69b9eae082fad79db08f1fce9905373232e6aea","last_reissued_at":"2026-05-18T01:08:59.316759Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:08:59.316759Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"quant-ph/0308038","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":"2026-05-18T01:08:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"hmznD2iitRiAXIp7DPxA3Zd2QmnZXbddJJcdfsjELw3cMqZyi9KmP1+CdIdVhblGXcuZak/5Czx/ykryLoQ2CQ==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:15:02.277383Z"},"content_sha256":"d5dcfe7ed823e540d5d8309dfcd9f08af8ea7d20e15d7c22cc155ef5398faf6b","schema_version":"1.0","event_id":"sha256:d5dcfe7ed823e540d5d8309dfcd9f08af8ea7d20e15d7c22cc155ef5398faf6b"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2003:O6SS3AELBN6W4VNMWVE7NG46VY","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Quantum Equilibrium and the Role of Operators as Observables in Quantum Theory","license":"","headline":"","cross_cats":[],"primary_cat":"quant-ph","authors_text":"Detlef D\\\"urr, Nino Zangh\\`{\\i}, Sheldon Goldstein","submitted_at":"2003-08-06T17:33:19Z","abstract_excerpt":"Bohmian mechnaics is the most naively obvious embedding imaginable of Schr\\\"odingers's equation into a completely coherent physical theory. It describes a world in which particles move in a highly non-Newtonian sort of way, one which may at first appear to have little to do with the spectrum of predictions of quantum mechanics. It turns out, however, that as a consequence of the defining dynamical equations of Bohmian mechanics, when a system has wave function $\\psi$ its configuration is typically random, with probability density $\\rho$ given by $|\\psi|^2$, the quantum equilibrium distribution"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"quant-ph/0308038","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":"2026-05-18T01:08:59Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"BV32JVB6p72W6S/+XvNA5J0WoYbwMT0rC9TtAX5lFKj6EygjUtrlRQ4oY8NVvIj9KJNDvepIXo/RInOlQe1NDg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-31T15:15:02.277955Z"},"content_sha256":"416e0e211803543de58a20364fca818bc44bdba87092db85fea77fbcefcd33cf","schema_version":"1.0","event_id":"sha256:416e0e211803543de58a20364fca818bc44bdba87092db85fea77fbcefcd33cf"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/O6SS3AELBN6W4VNMWVE7NG46VY/bundle.json","state_url":"https://pith.science/pith/O6SS3AELBN6W4VNMWVE7NG46VY/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/O6SS3AELBN6W4VNMWVE7NG46VY/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":"2026-05-31T15:15:02Z","links":{"resolver":"https://pith.science/pith/O6SS3AELBN6W4VNMWVE7NG46VY","bundle":"https://pith.science/pith/O6SS3AELBN6W4VNMWVE7NG46VY/bundle.json","state":"https://pith.science/pith/O6SS3AELBN6W4VNMWVE7NG46VY/state.json","well_known_bundle":"https://pith.science/.well-known/pith/O6SS3AELBN6W4VNMWVE7NG46VY/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2003:O6SS3AELBN6W4VNMWVE7NG46VY","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":"dd5ec630761ba52efcdb29cb87f7ea76f4332f93377a93479a1cd4784fde6c5a","cross_cats_sorted":[],"license":"","primary_cat":"quant-ph","submitted_at":"2003-08-06T17:33:19Z","title_canon_sha256":"97c5c8e22221251f8b270a57d90e49bb68c6ddf50208a617c08f2be735af7665"},"schema_version":"1.0","source":{"id":"quant-ph/0308038","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"quant-ph/0308038","created_at":"2026-05-18T01:08:59Z"},{"alias_kind":"arxiv_version","alias_value":"quant-ph/0308038v2","created_at":"2026-05-18T01:08:59Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.quant-ph/0308038","created_at":"2026-05-18T01:08:59Z"},{"alias_kind":"pith_short_12","alias_value":"O6SS3AELBN6W","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_16","alias_value":"O6SS3AELBN6W4VNM","created_at":"2026-05-18T12:25:52Z"},{"alias_kind":"pith_short_8","alias_value":"O6SS3AEL","created_at":"2026-05-18T12:25:52Z"}],"graph_snapshots":[{"event_id":"sha256:416e0e211803543de58a20364fca818bc44bdba87092db85fea77fbcefcd33cf","target":"graph","created_at":"2026-05-18T01:08:59Z","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":"Bohmian mechnaics is the most naively obvious embedding imaginable of Schr\\\"odingers's equation into a completely coherent physical theory. It describes a world in which particles move in a highly non-Newtonian sort of way, one which may at first appear to have little to do with the spectrum of predictions of quantum mechanics. It turns out, however, that as a consequence of the defining dynamical equations of Bohmian mechanics, when a system has wave function $\\psi$ its configuration is typically random, with probability density $\\rho$ given by $|\\psi|^2$, the quantum equilibrium distribution","authors_text":"Detlef D\\\"urr, Nino Zangh\\`{\\i}, Sheldon Goldstein","cross_cats":[],"headline":"","license":"","primary_cat":"quant-ph","submitted_at":"2003-08-06T17:33:19Z","title":"Quantum Equilibrium and the Role of Operators as Observables in Quantum Theory"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"quant-ph/0308038","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:d5dcfe7ed823e540d5d8309dfcd9f08af8ea7d20e15d7c22cc155ef5398faf6b","target":"record","created_at":"2026-05-18T01:08:59Z","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":"dd5ec630761ba52efcdb29cb87f7ea76f4332f93377a93479a1cd4784fde6c5a","cross_cats_sorted":[],"license":"","primary_cat":"quant-ph","submitted_at":"2003-08-06T17:33:19Z","title_canon_sha256":"97c5c8e22221251f8b270a57d90e49bb68c6ddf50208a617c08f2be735af7665"},"schema_version":"1.0","source":{"id":"quant-ph/0308038","kind":"arxiv","version":2}},"canonical_sha256":"77a52d808b0b7d6e55acb549f69b9eae082fad79db08f1fce9905373232e6aea","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"77a52d808b0b7d6e55acb549f69b9eae082fad79db08f1fce9905373232e6aea","first_computed_at":"2026-05-18T01:08:59.316759Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T01:08:59.316759Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"NED3bHUq0r0hZX6YfBu3iSA6/EmfQpGxAdRjutw4381Uojwn8ks0PB0VkdC9XWpBKPMfSRD0LykZ4uWdhhcvBg==","signature_status":"signed_v1","signed_at":"2026-05-18T01:08:59.317203Z","signed_message":"canonical_sha256_bytes"},"source_id":"quant-ph/0308038","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d5dcfe7ed823e540d5d8309dfcd9f08af8ea7d20e15d7c22cc155ef5398faf6b","sha256:416e0e211803543de58a20364fca818bc44bdba87092db85fea77fbcefcd33cf"],"state_sha256":"48725561d883e9ff1288f1d983535198695c50a18ad0e0cc800bfff1a317b2be"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9WS0359V4F7mesU/Eug9eSpvdRkjMzItftIG4HKsz0t18+gOPOL89rny1CCZPBW/1ZttEIj4bs8QeVk+Y4gvDA==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-31T15:15:02.282424Z","bundle_sha256":"c42152cb82d1a8e8f8ebd7611acd84e4bc1c8e49380e30861227e69006e39a98"}}