{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:ZKLUCS6BJHXMBSZ7C2AIHPAVES","short_pith_number":"pith:ZKLUCS6B","schema_version":"1.0","canonical_sha256":"ca97414bc149eec0cb3f168083bc1524af0c51c69145949ba3a3c5bc69423ff5","source":{"kind":"arxiv","id":"1812.05895","version":2},"attestation_state":"computed","paper":{"title":"Realization of density-dependent Peierls phases to engineer quantized gauge fields coupled to ultracold matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Frederik G\\\"org, Joaqu\\'in Minguzzi, Kilian Sandholzer, Michael Messer, R\\'emi Desbuquois, Tilman Esslinger","submitted_at":"2018-12-14T12:51:04Z","abstract_excerpt":"Gauge fields that appear in models of high-energy and condensed matter physics are dynamical quantum degrees of freedom due to their coupling to matter fields. Since the dynamics of these strongly correlated systems is hard to compute, it was proposed to implement this basic coupling mechanism in quantum simulation platforms with the ultimate goal to emulate lattice gauge theories. Here, we realize the fundamental ingredient for a density-dependent gauge field acting on ultracold fermions in an optical lattice by engineering non-trivial Peierls phases that depend on the site occupations. We pr"},"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":"1812.05895","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.quant-gas","submitted_at":"2018-12-14T12:51:04Z","cross_cats_sorted":["hep-lat","quant-ph"],"title_canon_sha256":"53264d245612c1d64640848a26efea193a68d96fce2b18e5309d9eecd5f47ff2","abstract_canon_sha256":"18465995bde700989828b472d5e0c9e970085af26c6a7c2e1bb4c7ded8a6ebcc"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:44:36.853378Z","signature_b64":"Q4xdXCgwb800Otf1s4yO5S6v1U2ahY6WIix25Bo06N4FFvBssG0lDKf0zJqrYo/hqgSIzgmjMjpl51GTzqKaBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca97414bc149eec0cb3f168083bc1524af0c51c69145949ba3a3c5bc69423ff5","last_reissued_at":"2026-07-05T00:44:36.852879Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:44:36.852879Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Realization of density-dependent Peierls phases to engineer quantized gauge fields coupled to ultracold matter","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","quant-ph"],"primary_cat":"cond-mat.quant-gas","authors_text":"Frederik G\\\"org, Joaqu\\'in Minguzzi, Kilian Sandholzer, Michael Messer, R\\'emi Desbuquois, Tilman Esslinger","submitted_at":"2018-12-14T12:51:04Z","abstract_excerpt":"Gauge fields that appear in models of high-energy and condensed matter physics are dynamical quantum degrees of freedom due to their coupling to matter fields. Since the dynamics of these strongly correlated systems is hard to compute, it was proposed to implement this basic coupling mechanism in quantum simulation platforms with the ultimate goal to emulate lattice gauge theories. Here, we realize the fundamental ingredient for a density-dependent gauge field acting on ultracold fermions in an optical lattice by engineering non-trivial Peierls phases that depend on the site occupations. We pr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1812.05895","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/1812.05895/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":"1812.05895","created_at":"2026-07-05T00:44:36.852944+00:00"},{"alias_kind":"arxiv_version","alias_value":"1812.05895v2","created_at":"2026-07-05T00:44:36.852944+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1812.05895","created_at":"2026-07-05T00:44:36.852944+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZKLUCS6BJHXM","created_at":"2026-07-05T00:44:36.852944+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZKLUCS6BJHXMBSZ7","created_at":"2026-07-05T00:44:36.852944+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZKLUCS6B","created_at":"2026-07-05T00:44:36.852944+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.15132","citing_title":"A minimal implementation of Yang-Mills theory on a digital quantum computer","ref_index":22,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES","json":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES.json","graph_json":"https://pith.science/api/pith-number/ZKLUCS6BJHXMBSZ7C2AIHPAVES/graph.json","events_json":"https://pith.science/api/pith-number/ZKLUCS6BJHXMBSZ7C2AIHPAVES/events.json","paper":"https://pith.science/paper/ZKLUCS6B"},"agent_actions":{"view_html":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES","download_json":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES.json","view_paper":"https://pith.science/paper/ZKLUCS6B","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1812.05895&json=true","fetch_graph":"https://pith.science/api/pith-number/ZKLUCS6BJHXMBSZ7C2AIHPAVES/graph.json","fetch_events":"https://pith.science/api/pith-number/ZKLUCS6BJHXMBSZ7C2AIHPAVES/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES/action/storage_attestation","attest_author":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES/action/author_attestation","sign_citation":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES/action/citation_signature","submit_replication":"https://pith.science/pith/ZKLUCS6BJHXMBSZ7C2AIHPAVES/action/replication_record"}},"created_at":"2026-07-05T00:44:36.852944+00:00","updated_at":"2026-07-05T00:44:36.852944+00:00"}