{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:AMVFD3VQJEBJ4FAIRFGZ7SCLIA","short_pith_number":"pith:AMVFD3VQ","schema_version":"1.0","canonical_sha256":"032a51eeb049029e1408894d9fc84b4039ba875b41dcc3599ec97ff69575333d","source":{"kind":"arxiv","id":"1607.08121","version":2},"attestation_state":"computed","paper":{"title":"Digital lattice gauge theories","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":"Alessandro Farace, Benni Reznik, Erez Zohar, J. Ignacio Cirac","submitted_at":"2016-07-27T14:30:46Z","abstract_excerpt":"We propose a general scheme for a digital construction of lattice gauge theories with dynamical fermions. In this method, the four-body interactions arising in models with $2+1$ dimensions and higher, are obtained stroboscopically, through a sequence of two-body interactions with ancillary degrees of freedom. This yields stronger interactions than the ones obtained through pertubative methods, as typically done in previous proposals, and removes an important bottleneck in the road towards experimental realizations. The scheme applies to generic gauge theories with Lie or finite symmetry groups"},"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":"1607.08121","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2016-07-27T14:30:46Z","cross_cats_sorted":["cond-mat.quant-gas","hep-lat","hep-th"],"title_canon_sha256":"126ea5c68f901ef52a9931d4d0600087a49645f11c6fe3279b521aad6f88eb5f","abstract_canon_sha256":"ecccb2d29534884b334eaab8a5a8a71199565d5d66722ad06ab0abe11d6db9ac"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:50:29.354301Z","signature_b64":"cfWENmLgnuANT112D2xAouyPX8TTyBbORQxNN0tcg32ASok1jHqQS5Axp4n75cFjO7evt98kIL0FuJsXg4JiDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"032a51eeb049029e1408894d9fc84b4039ba875b41dcc3599ec97ff69575333d","last_reissued_at":"2026-05-18T00:50:29.353635Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:50:29.353635Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Digital lattice gauge theories","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":"Alessandro Farace, Benni Reznik, Erez Zohar, J. Ignacio Cirac","submitted_at":"2016-07-27T14:30:46Z","abstract_excerpt":"We propose a general scheme for a digital construction of lattice gauge theories with dynamical fermions. In this method, the four-body interactions arising in models with $2+1$ dimensions and higher, are obtained stroboscopically, through a sequence of two-body interactions with ancillary degrees of freedom. This yields stronger interactions than the ones obtained through pertubative methods, as typically done in previous proposals, and removes an important bottleneck in the road towards experimental realizations. The scheme applies to generic gauge theories with Lie or finite symmetry groups"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1607.08121","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":"1607.08121","created_at":"2026-05-18T00:50:29.353730+00:00"},{"alias_kind":"arxiv_version","alias_value":"1607.08121v2","created_at":"2026-05-18T00:50:29.353730+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1607.08121","created_at":"2026-05-18T00:50:29.353730+00:00"},{"alias_kind":"pith_short_12","alias_value":"AMVFD3VQJEBJ","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_16","alias_value":"AMVFD3VQJEBJ4FAI","created_at":"2026-05-18T12:30:07.202191+00:00"},{"alias_kind":"pith_short_8","alias_value":"AMVFD3VQ","created_at":"2026-05-18T12:30:07.202191+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2604.26792","citing_title":"Fault-Tolerant Resource Comparison of Qudit and Qubit Encodings for Diagonal Quadratic Operators","ref_index":25,"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":25,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA","json":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA.json","graph_json":"https://pith.science/api/pith-number/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/graph.json","events_json":"https://pith.science/api/pith-number/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/events.json","paper":"https://pith.science/paper/AMVFD3VQ"},"agent_actions":{"view_html":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA","download_json":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA.json","view_paper":"https://pith.science/paper/AMVFD3VQ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1607.08121&json=true","fetch_graph":"https://pith.science/api/pith-number/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/graph.json","fetch_events":"https://pith.science/api/pith-number/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/action/storage_attestation","attest_author":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/action/author_attestation","sign_citation":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/action/citation_signature","submit_replication":"https://pith.science/pith/AMVFD3VQJEBJ4FAIRFGZ7SCLIA/action/replication_record"}},"created_at":"2026-05-18T00:50:29.353730+00:00","updated_at":"2026-05-18T00:50:29.353730+00:00"}