{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2019:2BLBNTKXJW5JGSS2RC7IWIYAIA","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"0cf675faf0adcfbb40721b13bb8623dc83f10d6cd22c560dd6da569cf6866876","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2019-01-21T22:28:14Z","title_canon_sha256":"49cfeddc6fdb34ac9d6d24ae6330868d92ec0762482e4e03918c863130836c16"},"schema_version":"1.0","source":{"id":"1901.07103","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1901.07103","created_at":"2026-07-05T00:22:36Z"},{"alias_kind":"arxiv_version","alias_value":"1901.07103v2","created_at":"2026-07-05T00:22:36Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1901.07103","created_at":"2026-07-05T00:22:36Z"},{"alias_kind":"pith_short_12","alias_value":"2BLBNTKXJW5J","created_at":"2026-07-05T00:22:36Z"},{"alias_kind":"pith_short_16","alias_value":"2BLBNTKXJW5JGSS2","created_at":"2026-07-05T00:22:36Z"},{"alias_kind":"pith_short_8","alias_value":"2BLBNTKX","created_at":"2026-07-05T00:22:36Z"}],"graph_snapshots":[{"event_id":"sha256:082b4e2e62059d2c8fd5dca8c55b88d79082a9293553325a38443cb1158d03f9","target":"graph","created_at":"2026-07-05T00:22:36Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/1901.07103/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Quantum simulation has the potential to investigate gauge theories in strongly-interacting regimes, which are up to now inaccessible through conventional numerical techniques. Here, we take a first step in this direction by implementing a Floquet-based method for studying $\\mathbb{Z}_2$ lattice gauge theories using two-component ultracold atoms in a double-well potential. For resonant periodic driving at the on-site interaction strength and an appropriate choice of the modulation parameters, the effective Floquet Hamiltonian exhibits $\\mathbb{Z}_2$ symmetry. We study the dynamics of the system","authors_text":"Christian Schweizer, Eugene Demler, Fabian Grusdt, Immanuel Bloch, Luca Barbiero, Monika Aidelsburger, Moritz Berngruber, Nathan Goldman","cross_cats":["cond-mat.str-el"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2019-01-21T22:28:14Z","title":"Floquet approach to $\\mathbb{Z}_{2}$ lattice gauge theories with ultracold atoms in optical lattices"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1901.07103","kind":"arxiv","version":2},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:c8eca928ec33a94be22f6cfa7f7b341156baa78b612c243267d11a7622f8628c","target":"record","created_at":"2026-07-05T00:22:36Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"0cf675faf0adcfbb40721b13bb8623dc83f10d6cd22c560dd6da569cf6866876","cross_cats_sorted":["cond-mat.str-el"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2019-01-21T22:28:14Z","title_canon_sha256":"49cfeddc6fdb34ac9d6d24ae6330868d92ec0762482e4e03918c863130836c16"},"schema_version":"1.0","source":{"id":"1901.07103","kind":"arxiv","version":2}},"canonical_sha256":"d05616cd574dba934a5a88be8b23004026050b9eb375dfda3e591020f0fc1f45","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"d05616cd574dba934a5a88be8b23004026050b9eb375dfda3e591020f0fc1f45","first_computed_at":"2026-07-05T00:22:36.889014Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T00:22:36.889014Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"vPQphwt6n05uR8CRIW59Dnqz1jyVm5KXDKNJ39heJbkdL1H+5jG4dcUqoH0ztuZs2M8AhWOrvmu0mcOkIfbAAQ==","signature_status":"signed_v1","signed_at":"2026-07-05T00:22:36.889521Z","signed_message":"canonical_sha256_bytes"},"source_id":"1901.07103","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:c8eca928ec33a94be22f6cfa7f7b341156baa78b612c243267d11a7622f8628c","sha256:082b4e2e62059d2c8fd5dca8c55b88d79082a9293553325a38443cb1158d03f9"],"state_sha256":"d9ae852394f04bd1a818abff061d524d077a310db700dbd7e1e9273e66c7e33f"}