{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:MJT6YQUFPU56L4MT2I3TTOQHKH","short_pith_number":"pith:MJT6YQUF","schema_version":"1.0","canonical_sha256":"6267ec42857d3be5f193d23739ba0751ca92412e5bdad303fc7684320d77c8cd","source":{"kind":"arxiv","id":"2211.01380","version":2},"attestation_state":"computed","paper":{"title":"Large-Scale $2+1$D $\\mathrm{U}(1)$ Gauge Theory with Dynamical Matter in a Cold-Atom Quantum Simulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat","hep-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Bing Yang, Ian P. McCulloch, Jad C. Halimeh, Jesse Osborne, Philipp Hauke","submitted_at":"2022-11-02T18:00:00Z","abstract_excerpt":"A major driver of quantum-simulator technology is the prospect of probing high-energy phenomena in synthetic quantum matter setups at a high level of control and tunability. Here, we propose an experimentally feasible realization of a large-scale $2+1$D $\\mathrm{U}(1)$ gauge theory with dynamical matter and gauge fields in a cold-atom quantum simulator with spinless bosons. We present the full mapping of the corresponding Gauss's law onto the bosonic computational basis. We then show that the target gauge theory can be faithfully realized and stabilized by an emergent gauge protection term in "},"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":"2211.01380","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2022-11-02T18:00:00Z","cross_cats_sorted":["cond-mat.str-el","hep-lat","hep-ph","quant-ph"],"title_canon_sha256":"3e5f371ff46682242020cfbe8631158fd9aab19ec6c50d1f2d63d39830be0bef","abstract_canon_sha256":"e44ce4e251953a8a24112fe606d8766418e6d688a595e97284ef70c74a69bfd5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:40:28.919308Z","signature_b64":"Qd5MvLMkfM1F0O6oOal60iy+iCPlABMJIAiA0gVP8UwVEL7j3u8o2J7H1QqehZFfS2akTCgUpiZSKXmwWQB0Dg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6267ec42857d3be5f193d23739ba0751ca92412e5bdad303fc7684320d77c8cd","last_reissued_at":"2026-07-05T11:40:28.918877Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:40:28.918877Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Large-Scale $2+1$D $\\mathrm{U}(1)$ Gauge Theory with Dynamical Matter in a Cold-Atom Quantum Simulator","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.str-el","hep-lat","hep-ph","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Bing Yang, Ian P. McCulloch, Jad C. Halimeh, Jesse Osborne, Philipp Hauke","submitted_at":"2022-11-02T18:00:00Z","abstract_excerpt":"A major driver of quantum-simulator technology is the prospect of probing high-energy phenomena in synthetic quantum matter setups at a high level of control and tunability. Here, we propose an experimentally feasible realization of a large-scale $2+1$D $\\mathrm{U}(1)$ gauge theory with dynamical matter and gauge fields in a cold-atom quantum simulator with spinless bosons. We present the full mapping of the corresponding Gauss's law onto the bosonic computational basis. We then show that the target gauge theory can be faithfully realized and stabilized by an emergent gauge protection term in "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2211.01380","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/2211.01380/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":"2211.01380","created_at":"2026-07-05T11:40:28.918941+00:00"},{"alias_kind":"arxiv_version","alias_value":"2211.01380v2","created_at":"2026-07-05T11:40:28.918941+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2211.01380","created_at":"2026-07-05T11:40:28.918941+00:00"},{"alias_kind":"pith_short_12","alias_value":"MJT6YQUFPU56","created_at":"2026-07-05T11:40:28.918941+00:00"},{"alias_kind":"pith_short_16","alias_value":"MJT6YQUFPU56L4MT","created_at":"2026-07-05T11:40:28.918941+00:00"},{"alias_kind":"pith_short_8","alias_value":"MJT6YQUF","created_at":"2026-07-05T11:40:28.918941+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.02756","citing_title":"Photonic Analog Quantum Simulation of (1+1)-Dimensional $U(1)$ Lattice Gauge Theory with Dynamical Matter","ref_index":70,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH","json":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH.json","graph_json":"https://pith.science/api/pith-number/MJT6YQUFPU56L4MT2I3TTOQHKH/graph.json","events_json":"https://pith.science/api/pith-number/MJT6YQUFPU56L4MT2I3TTOQHKH/events.json","paper":"https://pith.science/paper/MJT6YQUF"},"agent_actions":{"view_html":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH","download_json":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH.json","view_paper":"https://pith.science/paper/MJT6YQUF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2211.01380&json=true","fetch_graph":"https://pith.science/api/pith-number/MJT6YQUFPU56L4MT2I3TTOQHKH/graph.json","fetch_events":"https://pith.science/api/pith-number/MJT6YQUFPU56L4MT2I3TTOQHKH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH/action/storage_attestation","attest_author":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH/action/author_attestation","sign_citation":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH/action/citation_signature","submit_replication":"https://pith.science/pith/MJT6YQUFPU56L4MT2I3TTOQHKH/action/replication_record"}},"created_at":"2026-07-05T11:40:28.918941+00:00","updated_at":"2026-07-05T11:40:28.918941+00:00"}