{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:COG5SOISDJFGAAJAXQ3HYEZKOF","short_pith_number":"pith:COG5SOIS","schema_version":"1.0","canonical_sha256":"138dd939121a4a600120bc367c132a714fc851f9db8836e90b53aae389aeda54","source":{"kind":"arxiv","id":"2503.08866","version":2},"attestation_state":"computed","paper":{"title":"Quantum Circuits for SU(3) Lattice Gauge Theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","hep-th","quant-ph"],"primary_cat":"hep-lat","authors_text":"Andrew Lytle, Cian\\'an Conefrey-Shinozaki, Drishti Gupta, Enrico Rinaldi, Jason K. Elhaderi, Luis Hidalgo, Patrick Draper, Praveen Balaji","submitted_at":"2025-03-11T20:13:58Z","abstract_excerpt":"Lattice gauge theories in varying dimensions, lattice volumes, and truncations offer a rich family of targets for Hamiltonian simulation on quantum devices. In return, formulating quantum simulations can provide new ways of thinking about the quantum structure of gauge theories. In this work, we consider pure $SU(3)$ gauge theory in two and three spatial dimensions in a streamlined version of the electric basis. We use a formulation of the theory that balances locality of the Hamiltonian and size of the gauge-invariant state space, and we classically pre-compute dictionaries of plaquette opera"},"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":"2503.08866","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2025-03-11T20:13:58Z","cross_cats_sorted":["hep-ph","hep-th","quant-ph"],"title_canon_sha256":"64323f85fded903e86c011e791f779c3233da416cbbc9f67dd7b767a6e56621a","abstract_canon_sha256":"ad8b8727a89199cf6d2b8ade21568d37a2814ea10faaffbbb932856da4f91819"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T12:10:56.249014Z","signature_b64":"pOSY1trg0G1O1dUzQ46WRFGeo/ANRxPhFEW+LuEwEUiZs+sB5HYMBAdY6ccKCsLDPHlJctJ8CwVyVjHjeTBwAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"138dd939121a4a600120bc367c132a714fc851f9db8836e90b53aae389aeda54","last_reissued_at":"2026-07-05T12:10:56.248457Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T12:10:56.248457Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum Circuits for SU(3) Lattice Gauge Theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","hep-th","quant-ph"],"primary_cat":"hep-lat","authors_text":"Andrew Lytle, Cian\\'an Conefrey-Shinozaki, Drishti Gupta, Enrico Rinaldi, Jason K. Elhaderi, Luis Hidalgo, Patrick Draper, Praveen Balaji","submitted_at":"2025-03-11T20:13:58Z","abstract_excerpt":"Lattice gauge theories in varying dimensions, lattice volumes, and truncations offer a rich family of targets for Hamiltonian simulation on quantum devices. In return, formulating quantum simulations can provide new ways of thinking about the quantum structure of gauge theories. In this work, we consider pure $SU(3)$ gauge theory in two and three spatial dimensions in a streamlined version of the electric basis. We use a formulation of the theory that balances locality of the Hamiltonian and size of the gauge-invariant state space, and we classically pre-compute dictionaries of plaquette opera"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.08866","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2503.08866/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":"2503.08866","created_at":"2026-07-05T12:10:56.248525+00:00"},{"alias_kind":"arxiv_version","alias_value":"2503.08866v2","created_at":"2026-07-05T12:10:56.248525+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.08866","created_at":"2026-07-05T12:10:56.248525+00:00"},{"alias_kind":"pith_short_12","alias_value":"COG5SOISDJFG","created_at":"2026-07-05T12:10:56.248525+00:00"},{"alias_kind":"pith_short_16","alias_value":"COG5SOISDJFGAAJA","created_at":"2026-07-05T12:10:56.248525+00:00"},{"alias_kind":"pith_short_8","alias_value":"COG5SOIS","created_at":"2026-07-05T12:10:56.248525+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":10,"internal_anchor_count":0,"sample":[{"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":48,"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":41,"is_internal_anchor":false},{"citing_arxiv_id":"2605.22915","citing_title":"Unified resonant-manifold framework for dynamical quantum phase transitions","ref_index":174,"is_internal_anchor":false},{"citing_arxiv_id":"2605.22915","citing_title":"Unified resonant-manifold framework for dynamical quantum phase transitions","ref_index":164,"is_internal_anchor":false},{"citing_arxiv_id":"2605.20417","citing_title":"Quantum Simulation of Gauge Theories for Particle and Nuclear Physics","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2509.03586","citing_title":"Quantum simulation of out-of-equilibrium dynamics in gauge theories","ref_index":5,"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":173,"is_internal_anchor":false},{"citing_arxiv_id":"2603.23948","citing_title":"Local Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","ref_index":57,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07436","citing_title":"Observation of genuine $2+1$D string dynamics in a U$(1)$ lattice gauge theory with a tunable plaquette term on a trapped-ion quantum computer","ref_index":146,"is_internal_anchor":false},{"citing_arxiv_id":"2605.06907","citing_title":"A collider as a quantum computer","ref_index":20,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF","json":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF.json","graph_json":"https://pith.science/api/pith-number/COG5SOISDJFGAAJAXQ3HYEZKOF/graph.json","events_json":"https://pith.science/api/pith-number/COG5SOISDJFGAAJAXQ3HYEZKOF/events.json","paper":"https://pith.science/paper/COG5SOIS"},"agent_actions":{"view_html":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF","download_json":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF.json","view_paper":"https://pith.science/paper/COG5SOIS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2503.08866&json=true","fetch_graph":"https://pith.science/api/pith-number/COG5SOISDJFGAAJAXQ3HYEZKOF/graph.json","fetch_events":"https://pith.science/api/pith-number/COG5SOISDJFGAAJAXQ3HYEZKOF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF/action/storage_attestation","attest_author":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF/action/author_attestation","sign_citation":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF/action/citation_signature","submit_replication":"https://pith.science/pith/COG5SOISDJFGAAJAXQ3HYEZKOF/action/replication_record"}},"created_at":"2026-07-05T12:10:56.248525+00:00","updated_at":"2026-07-05T12:10:56.248525+00:00"}