{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:4X4YNAKBA7JOZSXWOBQGVDKK7O","short_pith_number":"pith:4X4YNAKB","schema_version":"1.0","canonical_sha256":"e5f986814107d2eccaf670606a8d4afb808475a075d4d2c016d7bee04a36f740","source":{"kind":"arxiv","id":"2509.25865","version":3},"attestation_state":"computed","paper":{"title":"Perturbation theory, irrep truncations, and state preparation methods for quantum simulations of SU(3) lattice gauge theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","quant-ph"],"primary_cat":"hep-lat","authors_text":"Andrew Lytle, Cianan Conefrey-Shinozaki, Drishti Gupta, Jason K. Elhaderi, Luis Hidalgo, Patrick Draper, Praveen Balaji","submitted_at":"2025-09-30T07:01:26Z","abstract_excerpt":"We study methods for efficient preparation of approximate ground states of $SU(3)$ lattice gauge theory on quantum hardware. Working in a variant of the electric basis, we introduce a refinement of the irrep truncation based on the energy density of site singlets, which provides a finer gradation of simulation complexity. Using strong-coupling perturbation theory as a guide, we develop simple ansatz circuits for ground state preparation and test them via classical simulation on small lattices, including the $2\\times 2$ plaquette lattice in $d=2$ and the cube in $d=3$. We contrast state fidelit"},"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":"2509.25865","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-lat","submitted_at":"2025-09-30T07:01:26Z","cross_cats_sorted":["hep-ph","quant-ph"],"title_canon_sha256":"81c8218f97b2b9aa0936468e32b5d4ec10a0df71cb88fe132adc36f990e158ce","abstract_canon_sha256":"abf2fe9897ac826a05353dd393bfc5f550fa2a335f7620a4f3ed1211761e51c6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-10T01:10:57.105109Z","signature_b64":"KdoQ4AeKZGS54wFZjYcFe//D208JO7CgALViDzV3/6eRkCn0nzn7aC5koAyoCLeP3P+MlOkJC30GEmMPjSZbAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e5f986814107d2eccaf670606a8d4afb808475a075d4d2c016d7bee04a36f740","last_reissued_at":"2026-06-10T01:10:57.104035Z","signature_status":"signed_v1","first_computed_at":"2026-06-10T01:10:57.104035Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Perturbation theory, irrep truncations, and state preparation methods for quantum simulations of SU(3) lattice gauge theory","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","quant-ph"],"primary_cat":"hep-lat","authors_text":"Andrew Lytle, Cianan Conefrey-Shinozaki, Drishti Gupta, Jason K. Elhaderi, Luis Hidalgo, Patrick Draper, Praveen Balaji","submitted_at":"2025-09-30T07:01:26Z","abstract_excerpt":"We study methods for efficient preparation of approximate ground states of $SU(3)$ lattice gauge theory on quantum hardware. Working in a variant of the electric basis, we introduce a refinement of the irrep truncation based on the energy density of site singlets, which provides a finer gradation of simulation complexity. Using strong-coupling perturbation theory as a guide, we develop simple ansatz circuits for ground state preparation and test them via classical simulation on small lattices, including the $2\\times 2$ plaquette lattice in $d=2$ and the cube in $d=3$. We contrast state fidelit"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2509.25865","kind":"arxiv","version":3},"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/2509.25865/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":"2509.25865","created_at":"2026-06-10T01:10:57.104179+00:00"},{"alias_kind":"arxiv_version","alias_value":"2509.25865v3","created_at":"2026-06-10T01:10:57.104179+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2509.25865","created_at":"2026-06-10T01:10:57.104179+00:00"},{"alias_kind":"pith_short_12","alias_value":"4X4YNAKBA7JO","created_at":"2026-06-10T01:10:57.104179+00:00"},{"alias_kind":"pith_short_16","alias_value":"4X4YNAKBA7JOZSXW","created_at":"2026-06-10T01:10:57.104179+00:00"},{"alias_kind":"pith_short_8","alias_value":"4X4YNAKB","created_at":"2026-06-10T01:10:57.104179+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":4,"sample":[{"citing_arxiv_id":"2605.22915","citing_title":"Unified resonant-manifold framework for dynamical quantum phase transitions","ref_index":163,"is_internal_anchor":true},{"citing_arxiv_id":"2603.23948","citing_title":"Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","ref_index":59,"is_internal_anchor":true},{"citing_arxiv_id":"2603.29091","citing_title":"Ether of Orbifolds","ref_index":65,"is_internal_anchor":true},{"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":145,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O","json":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O.json","graph_json":"https://pith.science/api/pith-number/4X4YNAKBA7JOZSXWOBQGVDKK7O/graph.json","events_json":"https://pith.science/api/pith-number/4X4YNAKBA7JOZSXWOBQGVDKK7O/events.json","paper":"https://pith.science/paper/4X4YNAKB"},"agent_actions":{"view_html":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O","download_json":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O.json","view_paper":"https://pith.science/paper/4X4YNAKB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2509.25865&json=true","fetch_graph":"https://pith.science/api/pith-number/4X4YNAKBA7JOZSXWOBQGVDKK7O/graph.json","fetch_events":"https://pith.science/api/pith-number/4X4YNAKBA7JOZSXWOBQGVDKK7O/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O/action/storage_attestation","attest_author":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O/action/author_attestation","sign_citation":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O/action/citation_signature","submit_replication":"https://pith.science/pith/4X4YNAKBA7JOZSXWOBQGVDKK7O/action/replication_record"}},"created_at":"2026-06-10T01:10:57.104179+00:00","updated_at":"2026-06-10T01:10:57.104179+00:00"}