{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:UGQ447BHBNJQMCOHL7N5Z4WDZ5","short_pith_number":"pith:UGQ447BH","schema_version":"1.0","canonical_sha256":"a1a1ce7c270b530609c75fdbdcf2c3cf425b41aa84d132da231817768b552d0d","source":{"kind":"arxiv","id":"2211.00017","version":2},"attestation_state":"computed","paper":{"title":"Non-Abelian Floquet Spin Liquids in a Digital Rydberg Simulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Marcin Kalinowski, Mikhail D. Lukin, Nishad Maskara","submitted_at":"2022-10-31T18:00:01Z","abstract_excerpt":"Understanding topological matter is an outstanding challenge across several disciplines of physical science. Programmable quantum simulators have emerged as a powerful approach to studying such systems. While quantum spin liquids of paradigmatic toric code type have recently been realized in the laboratory, controlled exploration of topological phases with non-abelian excitations remains an open problem. We introduce and analyze a new approach to simulating topological matter based on periodic driving. Specifically, we describe a model for a so-called Floquet spin liquid, obtained through a pe"},"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":"2211.00017","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2022-10-31T18:00:01Z","cross_cats_sorted":["cond-mat.str-el","physics.atom-ph"],"title_canon_sha256":"9de71efb93ff6e4fe584250b845acc534336dec17e355753277889e7b8342198","abstract_canon_sha256":"514818eb5b9cd327f0db8a813b28cde734d6b72811d0ec3c621722f9724df762"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:34:46.129109Z","signature_b64":"rAQqzKgFPcJpT/YdBId/nTD8hdbJTYbcDMJLMot4GN1Wi3rIg7+SGJQMKZt65hx/4iYFQwiBJ/e38ns35E5gCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"a1a1ce7c270b530609c75fdbdcf2c3cf425b41aa84d132da231817768b552d0d","last_reissued_at":"2026-07-05T06:34:46.128585Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:34:46.128585Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Non-Abelian Floquet Spin Liquids in a Digital Rydberg Simulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Marcin Kalinowski, Mikhail D. Lukin, Nishad Maskara","submitted_at":"2022-10-31T18:00:01Z","abstract_excerpt":"Understanding topological matter is an outstanding challenge across several disciplines of physical science. Programmable quantum simulators have emerged as a powerful approach to studying such systems. While quantum spin liquids of paradigmatic toric code type have recently been realized in the laboratory, controlled exploration of topological phases with non-abelian excitations remains an open problem. We introduce and analyze a new approach to simulating topological matter based on periodic driving. Specifically, we describe a model for a so-called Floquet spin liquid, obtained through a pe"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.00017","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/2211.00017/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":"2211.00017","created_at":"2026-07-05T06:34:46.128649+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.00017v2","created_at":"2026-07-05T06:34:46.128649+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.00017","created_at":"2026-07-05T06:34:46.128649+00:00"},{"alias_kind":"pith_short_12","alias_value":"UGQ447BHBNJQ","created_at":"2026-07-05T06:34:46.128649+00:00"},{"alias_kind":"pith_short_16","alias_value":"UGQ447BHBNJQMCOH","created_at":"2026-07-05T06:34:46.128649+00:00"},{"alias_kind":"pith_short_8","alias_value":"UGQ447BH","created_at":"2026-07-05T06:34:46.128649+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2302.08963","citing_title":"Order-by-disorder and emergent Kosterlitz-Thouless phase in triangular Rydberg array","ref_index":72,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5","json":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5.json","graph_json":"https://pith.science/api/pith-number/UGQ447BHBNJQMCOHL7N5Z4WDZ5/graph.json","events_json":"https://pith.science/api/pith-number/UGQ447BHBNJQMCOHL7N5Z4WDZ5/events.json","paper":"https://pith.science/paper/UGQ447BH"},"agent_actions":{"view_html":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5","download_json":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5.json","view_paper":"https://pith.science/paper/UGQ447BH","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.00017&json=true","fetch_graph":"https://pith.science/api/pith-number/UGQ447BHBNJQMCOHL7N5Z4WDZ5/graph.json","fetch_events":"https://pith.science/api/pith-number/UGQ447BHBNJQMCOHL7N5Z4WDZ5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5/action/storage_attestation","attest_author":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5/action/author_attestation","sign_citation":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5/action/citation_signature","submit_replication":"https://pith.science/pith/UGQ447BHBNJQMCOHL7N5Z4WDZ5/action/replication_record"}},"created_at":"2026-07-05T06:34:46.128649+00:00","updated_at":"2026-07-05T06:34:46.128649+00:00"}