{"paper":{"title":"$SU_q(2)$ Lattice Gauge Theory","license":"","headline":"","cross_cats":["hep-lat","math.QA","q-alg"],"primary_cat":"hep-th","authors_text":"A. Stern, G. Bimonte, P. Vitale","submitted_at":"1996-02-17T22:19:40Z","abstract_excerpt":"We reformulate the Hamiltonian approach to lattice gauge theories such that, at the classical level, the gauge group does not act canonically, but instead as a Poisson-Lie group. At the quantum level, it then gets promoted to a quantum group gauge symmetry. The theory depends on two parameters - the deformation parameter $\\lambda$ and the lattice spacing $a$. We show that the system of Kogut and Susskind is recovered when $\\lambda \\rightarrow 0$, while QCD is recovered in the continuum limit (for any $\\lambda$). We thus have the possibility of having a two parameter regularization of QCD."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/9602094","kind":"arxiv","version":1},"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"}