{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2022:6JRWTJPLCAWLQ2KGM56LEDKVM2","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":"e7d40aa7f650b6ddeac15b6e10f34bcb5a337e487910031151feedb853700e40","cross_cats_sorted":["hep-lat","hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-09-22T04:58:54Z","title_canon_sha256":"c16ccead398306b6f46d9f9a22ce043a0f701fc5b5665fa3c5cea464b988ef5c"},"schema_version":"1.0","source":{"id":"2209.10781","kind":"arxiv","version":3}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2209.10781","created_at":"2026-07-05T05:59:39Z"},{"alias_kind":"arxiv_version","alias_value":"2209.10781v3","created_at":"2026-07-05T05:59:39Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2209.10781","created_at":"2026-07-05T05:59:39Z"},{"alias_kind":"pith_short_12","alias_value":"6JRWTJPLCAWL","created_at":"2026-07-05T05:59:39Z"},{"alias_kind":"pith_short_16","alias_value":"6JRWTJPLCAWLQ2KG","created_at":"2026-07-05T05:59:39Z"},{"alias_kind":"pith_short_8","alias_value":"6JRWTJPL","created_at":"2026-07-05T05:59:39Z"}],"graph_snapshots":[{"event_id":"sha256:16d4fecd7877590b01568f0c923313bb37ce95c8f59f4bf294bbed4a1f9015f3","target":"graph","created_at":"2026-07-05T05:59:39Z","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/2209.10781/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"A framework for quantum simulations of real-time weak decays of hadrons and nuclei in a 2-flavor lattice theory in one spatial dimension is presented. A single generation of the Standard Model is found to require 16 qubits per spatial lattice site after mapping to spin operators via the Jordan-Wigner transformation. Both quantum chromodynamics and flavor-changing weak interactions are included in the dynamics, the latter through four-Fermi effective operators. Quantum circuits which implement time evolution in this lattice theory are developed and run on Quantinuum's H1-1 20-qubit trapped ion ","authors_text":"Ivan A. Chernyshev, Marc Illa, Martin J. Savage, Nikita A. Zemlevskiy, Roland C. Farrell, Sarah J. M. Powell","cross_cats":["hep-lat","hep-ph","nucl-th"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-09-22T04:58:54Z","title":"Preparations for Quantum Simulations of Quantum Chromodynamics in 1+1 Dimensions: (II) Single-Baryon $\\beta$-Decay in Real Time"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2209.10781","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":"sha256:573bf4419674dd1efe1abd643fe4a914c3b555a59a61739d39f73de5193e08c8","target":"record","created_at":"2026-07-05T05:59:39Z","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":"e7d40aa7f650b6ddeac15b6e10f34bcb5a337e487910031151feedb853700e40","cross_cats_sorted":["hep-lat","hep-ph","nucl-th"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-09-22T04:58:54Z","title_canon_sha256":"c16ccead398306b6f46d9f9a22ce043a0f701fc5b5665fa3c5cea464b988ef5c"},"schema_version":"1.0","source":{"id":"2209.10781","kind":"arxiv","version":3}},"canonical_sha256":"f26369a5eb102cb86946677cb20d5566a852c16d24b2ed7f05303ba7c1365513","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"f26369a5eb102cb86946677cb20d5566a852c16d24b2ed7f05303ba7c1365513","first_computed_at":"2026-07-05T05:59:39.756006Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T05:59:39.756006Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"BcVQDQ0R8vGJRqBI9LKf0sbXvjpFBG4qlHMX0wCZsX3sURxno3ZV3T7kV47muVolUlnNDKqpIIEoepQq3+f+Bw==","signature_status":"signed_v1","signed_at":"2026-07-05T05:59:39.756458Z","signed_message":"canonical_sha256_bytes"},"source_id":"2209.10781","source_kind":"arxiv","source_version":3}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:573bf4419674dd1efe1abd643fe4a914c3b555a59a61739d39f73de5193e08c8","sha256:16d4fecd7877590b01568f0c923313bb37ce95c8f59f4bf294bbed4a1f9015f3"],"state_sha256":"74390be9e364d68df8a54a9d33fadad29a24951e85b9bf0f4de09f7f76e8ce11"}