{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2026:QTRARDMLWB32Y7SFQLBOMG7ZGD","merge_version":"pith-open-graph-merge-v1","event_count":3,"valid_event_count":3,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"651d07726319a125bbe3e79a4496a8721272e0b1d666eefa5fce09c7faf6899e","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-06T20:26:27Z","title_canon_sha256":"bb2b6c8948e92d74a939ad9b408c63904bdf34ceb95af10386e0b5b878533807"},"schema_version":"1.0","source":{"id":"2608.06570","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2608.06570","created_at":"2026-08-10T01:11:18Z"},{"alias_kind":"arxiv_version","alias_value":"2608.06570v1","created_at":"2026-08-10T01:11:18Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.06570","created_at":"2026-08-10T01:11:18Z"},{"alias_kind":"pith_short_12","alias_value":"QTRARDMLWB32","created_at":"2026-08-10T01:11:18Z"},{"alias_kind":"pith_short_16","alias_value":"QTRARDMLWB32Y7SF","created_at":"2026-08-10T01:11:18Z"},{"alias_kind":"pith_short_8","alias_value":"QTRARDML","created_at":"2026-08-10T01:11:18Z"}],"graph_snapshots":[{"event_id":"sha256:343080863b14f28670546c72eff275c9bf23d9585db2f8bf735fdbf16b5a77d4","target":"graph","created_at":"2026-08-10T01:11:18Z","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/2608.06570/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"The quantum lattice Boltzmann (QLB) scheme of Succi and Dellar advances a four-component Dirac spinor on a lattice by a fixed sequence of local, exactly norm-preserving operations: a basis rotation, a collision, a streaming shift, and the inverse rotation. This unitarity is a structural property of the scheme, not an approximation, which suggests that a QLB time step should map onto a sequence of quantum gates. Here we make that mapping explicit. We give a gate-level construction of every operation of the three-dimensional Dirac QLB scheme: the fixed rotation gates, the collision gate, the str","authors_text":"Ethan Young, Kevin Griffin, Michael Martin, Nilesh Sawant","cross_cats":["cond-mat.stat-mech","math-ph","math.MP","physics.comp-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-06T20:26:27Z","title":"Exact quantum circuits for lattice Boltzmann realization of the Dirac equation"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.06570","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":"sha256:860b90f1eb9b56ccf1edeae436a7b89444c75e874c63d5b53959a4596a7166d7","target":"record","created_at":"2026-08-10T01:11:18Z","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":"651d07726319a125bbe3e79a4496a8721272e0b1d666eefa5fce09c7faf6899e","cross_cats_sorted":["cond-mat.stat-mech","math-ph","math.MP","physics.comp-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2026-08-06T20:26:27Z","title_canon_sha256":"bb2b6c8948e92d74a939ad9b408c63904bdf34ceb95af10386e0b5b878533807"},"schema_version":"1.0","source":{"id":"2608.06570","kind":"arxiv","version":1}},"canonical_sha256":"84e2088d8bb077ac7e4582c2e61bf930d28a1c93757058fbfb50c553a9573ba2","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"84e2088d8bb077ac7e4582c2e61bf930d28a1c93757058fbfb50c553a9573ba2","first_computed_at":"2026-08-10T01:11:18.852842Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-08-10T01:11:18.852842Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"xEGD/tXSV9yf7QJizhcbMpZrij4BFP6qSAQpaAJv7zADQc0C4ohPMyKNKyGdQBkOGuXU3LBNrjfPmmViXqNCDg==","signature_status":"signed_v1","signed_at":"2026-08-10T01:11:18.856187Z","signed_message":"canonical_sha256_bytes"},"source_id":"2608.06570","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:860b90f1eb9b56ccf1edeae436a7b89444c75e874c63d5b53959a4596a7166d7","sha256:343080863b14f28670546c72eff275c9bf23d9585db2f8bf735fdbf16b5a77d4","sha256:cb629ad27f96092abb3a7255002c643865b92f659e2b040c2a511ba23bcf03c7"],"state_sha256":"ed3159751c0ef02403c99740468dd7bdf9f61a81e667b1367517883b25eb5451"}