{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:LCU537SDIJBOM3TQG4RTMWWK6P","short_pith_number":"pith:LCU537SD","schema_version":"1.0","canonical_sha256":"58a9ddfe434242e66e703723365acaf3fc239582af5721409872bd8cb36146d6","source":{"kind":"arxiv","id":"2402.10265","version":4},"attestation_state":"computed","paper":{"title":"Quantum Simulation of SU(3) Lattice Yang Mills Theory at Leading Order in Large N","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","quant-ph"],"primary_cat":"hep-ph","authors_text":"Anthony N. Ciavarella, Christian W. Bauer","submitted_at":"2024-02-15T19:00:01Z","abstract_excerpt":"Quantum simulations of the dynamics of QCD have been limited by the complexities of mapping the continuous gauge fields onto quantum computers. By parametrizing the gauge invariant Hilbert space in terms of plaquette degrees of freedom, we show how the Hilbert space and interactions can be expanded in inverse powers of N_c. At leading order in this expansion, the Hamiltonian simplifies dramatically, both in the required size of the Hilbert space as well as the type of interactions involved. Adding a truncation of the resulting Hilbert space in terms of local energy states we give explicit cons"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2402.10265","kind":"arxiv","version":4},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-02-15T19:00:01Z","cross_cats_sorted":["hep-lat","quant-ph"],"title_canon_sha256":"2d4ecea9045c43db88638d7267f10372a3da1d8a32f8819661a9341f5c77a942","abstract_canon_sha256":"8f42e1bdc5ae625e52d56540cce127f9f80e2e7d73fdf2ea253a3c546fc1cd77"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:59:26.071720Z","signature_b64":"g0W0torOb2g75Sb2vO9v4YjwW/LkEmoZzt0s4r8syyF/X1Q2UHo39Z5az2j78Av/WFwenMjRoGWwEmhPaWz4Cg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"58a9ddfe434242e66e703723365acaf3fc239582af5721409872bd8cb36146d6","last_reissued_at":"2026-07-05T08:59:26.071172Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:59:26.071172Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Simulation of SU(3) Lattice Yang Mills Theory at Leading Order in Large N","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","quant-ph"],"primary_cat":"hep-ph","authors_text":"Anthony N. Ciavarella, Christian W. Bauer","submitted_at":"2024-02-15T19:00:01Z","abstract_excerpt":"Quantum simulations of the dynamics of QCD have been limited by the complexities of mapping the continuous gauge fields onto quantum computers. By parametrizing the gauge invariant Hilbert space in terms of plaquette degrees of freedom, we show how the Hilbert space and interactions can be expanded in inverse powers of N_c. At leading order in this expansion, the Hamiltonian simplifies dramatically, both in the required size of the Hilbert space as well as the type of interactions involved. Adding a truncation of the resulting Hilbert space in terms of local energy states we give explicit cons"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.10265","kind":"arxiv","version":4},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2402.10265/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"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"},"aliases":[{"alias_kind":"arxiv","alias_value":"2402.10265","created_at":"2026-07-05T08:59:26.071230+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.10265v4","created_at":"2026-07-05T08:59:26.071230+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.10265","created_at":"2026-07-05T08:59:26.071230+00:00"},{"alias_kind":"pith_short_12","alias_value":"LCU537SDIJBO","created_at":"2026-07-05T08:59:26.071230+00:00"},{"alias_kind":"pith_short_16","alias_value":"LCU537SDIJBOM3TQ","created_at":"2026-07-05T08:59:26.071230+00:00"},{"alias_kind":"pith_short_8","alias_value":"LCU537SD","created_at":"2026-07-05T08:59:26.071230+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":13,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.19601","citing_title":"String dynamics of a (2+1)D U(1) quantum link model on a digital quantum computer","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02756","citing_title":"Photonic Analog Quantum Simulation of (1+1)-Dimensional $U(1)$ Lattice Gauge Theory with Dynamical Matter","ref_index":47,"is_internal_anchor":false},{"citing_arxiv_id":"2606.02574","citing_title":"Quantum Simulation of Nucleon-Antinucleon Interaction in Large-$N$ QCD$_2$ on an IBM Quantum Nighthawk Processor","ref_index":34,"is_internal_anchor":false},{"citing_arxiv_id":"2605.15076","citing_title":"Deforming the Trail: Baseline Quantum Circuitry for $\\text{SU(2)}_k$ Lattice Gauge Theory","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2605.20417","citing_title":"Quantum Simulation of Gauge Theories for Particle and Nuclear Physics","ref_index":48,"is_internal_anchor":false},{"citing_arxiv_id":"2512.05210","citing_title":"A Framework for Quantum Simulations of Energy-Loss and Hadronization in Non-Abelian Gauge Theories: SU(2) Lattice Gauge Theory in 1+1D","ref_index":57,"is_internal_anchor":false},{"citing_arxiv_id":"2601.08825","citing_title":"The Quantum Complexity of String Breaking in the Schwinger Model","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2602.02344","citing_title":"Large Nc Truncations for SU(Nc) Lattice Yang-Mills Theory with Fermions","ref_index":147,"is_internal_anchor":false},{"citing_arxiv_id":"2603.23948","citing_title":"Local Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2603.29091","citing_title":"Ether of Orbifolds","ref_index":69,"is_internal_anchor":false},{"citing_arxiv_id":"2605.04210","citing_title":"Nonlocal Nonstabilizerness from Holographic Schwinger Pair Production","ref_index":54,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06907","citing_title":"A collider as a quantum computer","ref_index":19,"is_internal_anchor":false},{"citing_arxiv_id":"2604.15132","citing_title":"A minimal implementation of Yang-Mills theory on a digital quantum computer","ref_index":43,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P","json":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P.json","graph_json":"https://pith.science/api/pith-number/LCU537SDIJBOM3TQG4RTMWWK6P/graph.json","events_json":"https://pith.science/api/pith-number/LCU537SDIJBOM3TQG4RTMWWK6P/events.json","paper":"https://pith.science/paper/LCU537SD"},"agent_actions":{"view_html":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P","download_json":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P.json","view_paper":"https://pith.science/paper/LCU537SD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.10265&json=true","fetch_graph":"https://pith.science/api/pith-number/LCU537SDIJBOM3TQG4RTMWWK6P/graph.json","fetch_events":"https://pith.science/api/pith-number/LCU537SDIJBOM3TQG4RTMWWK6P/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P/action/timestamp_anchor","attest_storage":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P/action/storage_attestation","attest_author":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P/action/author_attestation","sign_citation":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P/action/citation_signature","submit_replication":"https://pith.science/pith/LCU537SDIJBOM3TQG4RTMWWK6P/action/replication_record"}},"created_at":"2026-07-05T08:59:26.071230+00:00","updated_at":"2026-07-05T08:59:26.071230+00:00"}