{"paper":{"title":"Dual infrared limits of 6d $\\cal N$=(2,0) theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["math-ph","math.MP"],"primary_cat":"hep-th","authors_text":"Alexander D. Popov, Olaf Lechtenfeld","submitted_at":"2018-11-08T19:11:06Z","abstract_excerpt":"Compactifying type $A_{N-1}$ 6d ${\\cal N}{=}(2,0)$ supersymmetric CFT on a product manifold $M^4\\times\\Sigma^2=M^3\\times\\tilde{S}^1\\times S^1\\times{\\cal I}$ either over $S^1$ or over $\\tilde{S}^1$ leads to maximally supersymmetric 5d gauge theories on $M^4\\times{\\cal I}$ or on $M^3\\times\\Sigma^2$, respectively. Choosing the radii of $S^1$ and $\\tilde{S}^1$ inversely proportional to each other, these 5d gauge theories are dual to one another since their coupling constants $e^2$ and $\\tilde{e}^2$ are proportional to those radii respectively. We consider their non-Abelian but non-supersymmetric e"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1811.03649","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"}