{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:ABK5Z6ACJNARI7SBWWAPJ67U47","short_pith_number":"pith:ABK5Z6AC","schema_version":"1.0","canonical_sha256":"0055dcf8024b41147e41b580f4fbf4e7e65dfc3d97e12c00727bc3eeb7cefba7","source":{"kind":"arxiv","id":"2203.15541","version":2},"attestation_state":"computed","paper":{"title":"Hardware efficient quantum simulation of non-abelian gauge theories with qudits on Rydberg platforms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat"],"primary_cat":"quant-ph","authors_text":"Barbara Kraus, Daniel Gonz\\'alez-Cuadra, Jose Carrasco, Peter Zoller, Torsten V. Zache","submitted_at":"2022-03-29T13:26:37Z","abstract_excerpt":"Non-abelian gauge theories underlie our understanding of fundamental forces in nature, and developing tailored quantum hardware and algorithms to simulate them is an outstanding challenge in the rapidly evolving field of quantum simulation. Here we take an approach where gauge fields, discretized in spacetime, are represented by qudits and are time-evolved in Trotter steps with multiqudit quantum gates. This maps naturally and hardware-efficiently to an architecture based on Rydberg tweezer arrays, where long-lived internal atomic states represent qudits, and the required quantum gates are per"},"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":"2203.15541","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-03-29T13:26:37Z","cross_cats_sorted":["cond-mat.quant-gas","hep-lat"],"title_canon_sha256":"07f5ca984ee767f49681bbe2fd10e7254d8c7cd32d668f640d2a98a76b2ca003","abstract_canon_sha256":"4d1a168f7376797a8212f0b364862f2dd24ecc3ade0829a5e992af8e28685e41"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T05:31:47.590293Z","signature_b64":"ntCjLpoPDGWG8GvadsXYuCtcH9XczATstk9bkZ2iZt6eufoFDaAkpYB37KhpWtazXO7S1k2O6d1hTAq3zbRUAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0055dcf8024b41147e41b580f4fbf4e7e65dfc3d97e12c00727bc3eeb7cefba7","last_reissued_at":"2026-07-05T05:31:47.589810Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T05:31:47.589810Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hardware efficient quantum simulation of non-abelian gauge theories with qudits on Rydberg platforms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat"],"primary_cat":"quant-ph","authors_text":"Barbara Kraus, Daniel Gonz\\'alez-Cuadra, Jose Carrasco, Peter Zoller, Torsten V. Zache","submitted_at":"2022-03-29T13:26:37Z","abstract_excerpt":"Non-abelian gauge theories underlie our understanding of fundamental forces in nature, and developing tailored quantum hardware and algorithms to simulate them is an outstanding challenge in the rapidly evolving field of quantum simulation. Here we take an approach where gauge fields, discretized in spacetime, are represented by qudits and are time-evolved in Trotter steps with multiqudit quantum gates. This maps naturally and hardware-efficiently to an architecture based on Rydberg tweezer arrays, where long-lived internal atomic states represent qudits, and the required quantum gates are per"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2203.15541","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/2203.15541/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":"2203.15541","created_at":"2026-07-05T05:31:47.589872+00:00"},{"alias_kind":"arxiv_version","alias_value":"2203.15541v2","created_at":"2026-07-05T05:31:47.589872+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2203.15541","created_at":"2026-07-05T05:31:47.589872+00:00"},{"alias_kind":"pith_short_12","alias_value":"ABK5Z6ACJNAR","created_at":"2026-07-05T05:31:47.589872+00:00"},{"alias_kind":"pith_short_16","alias_value":"ABK5Z6ACJNARI7SB","created_at":"2026-07-05T05:31:47.589872+00:00"},{"alias_kind":"pith_short_8","alias_value":"ABK5Z6AC","created_at":"2026-07-05T05:31:47.589872+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.15076","citing_title":"Deforming the Trail: Baseline Quantum Circuitry for $\\text{SU(2)}_k$ Lattice Gauge Theory","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26792","citing_title":"Fault-Tolerant Resource Comparison of Qudit and Qubit Encodings for Diagonal Quadratic Operators","ref_index":38,"is_internal_anchor":false},{"citing_arxiv_id":"2605.20417","citing_title":"Quantum Simulation of Gauge Theories for Particle and Nuclear Physics","ref_index":74,"is_internal_anchor":false},{"citing_arxiv_id":"2603.23948","citing_title":"Local Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","ref_index":92,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26792","citing_title":"Fault-Tolerant Resource Comparison of Qudit and Qubit Encodings for Diagonal Quadratic Operators","ref_index":38,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47","json":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47.json","graph_json":"https://pith.science/api/pith-number/ABK5Z6ACJNARI7SBWWAPJ67U47/graph.json","events_json":"https://pith.science/api/pith-number/ABK5Z6ACJNARI7SBWWAPJ67U47/events.json","paper":"https://pith.science/paper/ABK5Z6AC"},"agent_actions":{"view_html":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47","download_json":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47.json","view_paper":"https://pith.science/paper/ABK5Z6AC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2203.15541&json=true","fetch_graph":"https://pith.science/api/pith-number/ABK5Z6ACJNARI7SBWWAPJ67U47/graph.json","fetch_events":"https://pith.science/api/pith-number/ABK5Z6ACJNARI7SBWWAPJ67U47/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47/action/storage_attestation","attest_author":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47/action/author_attestation","sign_citation":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47/action/citation_signature","submit_replication":"https://pith.science/pith/ABK5Z6ACJNARI7SBWWAPJ67U47/action/replication_record"}},"created_at":"2026-07-05T05:31:47.589872+00:00","updated_at":"2026-07-05T05:31:47.589872+00:00"}