{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:ZJCEH7U4QGIMLI6PTS67KHEJTU","short_pith_number":"pith:ZJCEH7U4","schema_version":"1.0","canonical_sha256":"ca4443fe9c8190c5a3cf9cbdf51c899d3a1b1351b735b9e89f36b1cac520eccb","source":{"kind":"arxiv","id":"1211.2241","version":2},"attestation_state":"computed","paper":{"title":"A cold-atom quantum simulator for SU(2) Yang-Mills lattice gauge theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat","hep-th"],"primary_cat":"quant-ph","authors_text":"Benni Reznik, Erez Zohar, J. Ignacio Cirac","submitted_at":"2012-11-09T21:07:47Z","abstract_excerpt":"Non-abelian gauge theories play an important role in the standard model of particle physics, and unfold a partially unexplored world of exciting physical phenomena. In this letter, we suggest a realization of a non-abelian lattice gauge theory - SU(2) Yang-Mills in 1+1 dimensions, using ultracold atoms. Remarkably, and in contrast to previous proposals, in our model gauge invariance is a direct consequence of angular momentum conservation and thus is fundamental and robust. Our proposal may serve as well as a starting point for higher dimensional realizations."},"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":"1211.2241","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2012-11-09T21:07:47Z","cross_cats_sorted":["cond-mat.quant-gas","hep-lat","hep-th"],"title_canon_sha256":"012492e2346574a9286cd74b03a9b530c462c4ffb12d3032cf9c9863bd0e9ef4","abstract_canon_sha256":"8a2f7f2f8f0e248f0a04c3f30c5143b03942b81f60463d14bfde7ed4de5f2522"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:30:12.239814Z","signature_b64":"5Jccf9LvClIjm2B+TG1yACYS8JBy7THIj/UllbPZE1AdRFyhTXU99BRYSqXekTLvp7XrxuBRqwPTTF2jLS2sDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ca4443fe9c8190c5a3cf9cbdf51c899d3a1b1351b735b9e89f36b1cac520eccb","last_reissued_at":"2026-05-18T03:30:12.239265Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:30:12.239265Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"A cold-atom quantum simulator for SU(2) Yang-Mills lattice gauge theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","hep-lat","hep-th"],"primary_cat":"quant-ph","authors_text":"Benni Reznik, Erez Zohar, J. Ignacio Cirac","submitted_at":"2012-11-09T21:07:47Z","abstract_excerpt":"Non-abelian gauge theories play an important role in the standard model of particle physics, and unfold a partially unexplored world of exciting physical phenomena. In this letter, we suggest a realization of a non-abelian lattice gauge theory - SU(2) Yang-Mills in 1+1 dimensions, using ultracold atoms. Remarkably, and in contrast to previous proposals, in our model gauge invariance is a direct consequence of angular momentum conservation and thus is fundamental and robust. Our proposal may serve as well as a starting point for higher dimensional realizations."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1211.2241","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":""},"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":"1211.2241","created_at":"2026-05-18T03:30:12.239367+00:00"},{"alias_kind":"arxiv_version","alias_value":"1211.2241v2","created_at":"2026-05-18T03:30:12.239367+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1211.2241","created_at":"2026-05-18T03:30:12.239367+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZJCEH7U4QGIM","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZJCEH7U4QGIMLI6P","created_at":"2026-05-18T12:27:30.460161+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZJCEH7U4","created_at":"2026-05-18T12:27:30.460161+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2604.26792","citing_title":"Fault-Tolerant Resource Comparison of Qudit and Qubit Encodings for Diagonal Quadratic Operators","ref_index":35,"is_internal_anchor":true},{"citing_arxiv_id":"2602.22313","citing_title":"Quantum simulation of massive Thirring and Gross--Neveu models for arbitrary number of flavors","ref_index":11,"is_internal_anchor":true},{"citing_arxiv_id":"2603.23948","citing_title":"Thermalization of SU(2) Lattice Gauge Fields on Quantum Computers","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2604.26792","citing_title":"Fault-Tolerant Resource Comparison of Qudit and Qubit Encodings for Diagonal Quadratic Operators","ref_index":35,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU","json":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU.json","graph_json":"https://pith.science/api/pith-number/ZJCEH7U4QGIMLI6PTS67KHEJTU/graph.json","events_json":"https://pith.science/api/pith-number/ZJCEH7U4QGIMLI6PTS67KHEJTU/events.json","paper":"https://pith.science/paper/ZJCEH7U4"},"agent_actions":{"view_html":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU","download_json":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU.json","view_paper":"https://pith.science/paper/ZJCEH7U4","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1211.2241&json=true","fetch_graph":"https://pith.science/api/pith-number/ZJCEH7U4QGIMLI6PTS67KHEJTU/graph.json","fetch_events":"https://pith.science/api/pith-number/ZJCEH7U4QGIMLI6PTS67KHEJTU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU/action/storage_attestation","attest_author":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU/action/author_attestation","sign_citation":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU/action/citation_signature","submit_replication":"https://pith.science/pith/ZJCEH7U4QGIMLI6PTS67KHEJTU/action/replication_record"}},"created_at":"2026-05-18T03:30:12.239367+00:00","updated_at":"2026-05-18T03:30:12.239367+00:00"}