{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:D366BM7VJNOCTFUS3GTYH3U6OC","short_pith_number":"pith:D366BM7V","schema_version":"1.0","canonical_sha256":"1efde0b3f54b5c299692d9a783ee9e70b937a86b9f58d040d6d17e3ea13a432e","source":{"kind":"arxiv","id":"2603.15820","version":2},"attestation_state":"computed","paper":{"title":"Quantum simulation of lattice gauge theories coupled to fermionic matter via anyonic regularization","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat"],"primary_cat":"quant-ph","authors_text":"Mason L. Rhodes, Riley W. Chien, Shivesh Pathak","submitted_at":"2026-03-16T18:51:41Z","abstract_excerpt":"The optimal regularization of infinite-dimensional gauge-field degrees of freedom is a central open problem in the simulation of lattice gauge theories on quantum computers. Here, we consider regularizing the gauge field by replacing the gauge group $G$ with a braided fusion category whose objects correspond to Wilson lines of the associated Chern-Simons theory $G_k$, with the level $k$ serving as the regularization parameter. We demonstrate how to couple these regularized gauge groups to fermionic matter using the framework of fusion surface models, which treats matter and gauge field excitat"},"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":"2603.15820","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"quant-ph","submitted_at":"2026-03-16T18:51:41Z","cross_cats_sorted":["cond-mat.str-el","hep-lat"],"title_canon_sha256":"df25f800ecdff442bd0c38f2d3c2324975532d81693f1513b63eda69063ab9c9","abstract_canon_sha256":"979df0877efd870df9ce797517086640814a49ba56eeb5f4a73a7fc1ce431be2"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-03T01:05:11.625050Z","signature_b64":"cDkC6/SiYCGnE++1V01owuC2/gFYFs5g/bU5h/euRoruY0TGD/PoLRGEwSbYYgnC2XDhv33HXeDZwDh5gjh4Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1efde0b3f54b5c299692d9a783ee9e70b937a86b9f58d040d6d17e3ea13a432e","last_reissued_at":"2026-06-03T01:05:11.624503Z","signature_status":"signed_v1","first_computed_at":"2026-06-03T01:05:11.624503Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quantum simulation of lattice gauge theories coupled to fermionic matter via anyonic regularization","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat"],"primary_cat":"quant-ph","authors_text":"Mason L. Rhodes, Riley W. Chien, Shivesh Pathak","submitted_at":"2026-03-16T18:51:41Z","abstract_excerpt":"The optimal regularization of infinite-dimensional gauge-field degrees of freedom is a central open problem in the simulation of lattice gauge theories on quantum computers. Here, we consider regularizing the gauge field by replacing the gauge group $G$ with a braided fusion category whose objects correspond to Wilson lines of the associated Chern-Simons theory $G_k$, with the level $k$ serving as the regularization parameter. We demonstrate how to couple these regularized gauge groups to fermionic matter using the framework of fusion surface models, which treats matter and gauge field excitat"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2603.15820","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/2603.15820/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":"2603.15820","created_at":"2026-06-03T01:05:11.624561+00:00"},{"alias_kind":"arxiv_version","alias_value":"2603.15820v2","created_at":"2026-06-03T01:05:11.624561+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2603.15820","created_at":"2026-06-03T01:05:11.624561+00:00"},{"alias_kind":"pith_short_12","alias_value":"D366BM7VJNOC","created_at":"2026-06-03T01:05:11.624561+00:00"},{"alias_kind":"pith_short_16","alias_value":"D366BM7VJNOCTFUS","created_at":"2026-06-03T01:05:11.624561+00:00"},{"alias_kind":"pith_short_8","alias_value":"D366BM7V","created_at":"2026-06-03T01:05:11.624561+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2603.29091","citing_title":"Ether of Orbifolds","ref_index":14,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC","json":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC.json","graph_json":"https://pith.science/api/pith-number/D366BM7VJNOCTFUS3GTYH3U6OC/graph.json","events_json":"https://pith.science/api/pith-number/D366BM7VJNOCTFUS3GTYH3U6OC/events.json","paper":"https://pith.science/paper/D366BM7V"},"agent_actions":{"view_html":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC","download_json":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC.json","view_paper":"https://pith.science/paper/D366BM7V","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2603.15820&json=true","fetch_graph":"https://pith.science/api/pith-number/D366BM7VJNOCTFUS3GTYH3U6OC/graph.json","fetch_events":"https://pith.science/api/pith-number/D366BM7VJNOCTFUS3GTYH3U6OC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC/action/storage_attestation","attest_author":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC/action/author_attestation","sign_citation":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC/action/citation_signature","submit_replication":"https://pith.science/pith/D366BM7VJNOCTFUS3GTYH3U6OC/action/replication_record"}},"created_at":"2026-06-03T01:05:11.624561+00:00","updated_at":"2026-06-03T01:05:11.624561+00:00"}