{"title":"Double Poisson brackets and involutive representation spaces","authors":"Grigori Olshanski, Nikita Safonkin","doi":"10.1007/s11005-024-01782-3","DOIUrl":null,"url":null,"abstract":"<div><p>Let <span>\\(\\Bbbk \\)</span> be an algebraically closed field of characteristic 0 and <i>A</i> be a finitely generated associative <span>\\(\\Bbbk \\)</span>-algebra, in general noncommutative. One assigns to <i>A</i> a sequence of commutative <span>\\(\\Bbbk \\)</span>-algebras <span>\\(\\mathcal {O}(A,d)\\)</span>, <span>\\(d=1,2,3,\\dots \\)</span>, where <span>\\(\\mathcal {O}(A,d)\\)</span> is the coordinate ring of the space <span>\\({\\text {Rep}}(A,d)\\)</span> of <i>d</i>-dimensional representations of the algebra <i>A</i>. A <i>double Poisson bracket</i> on <i>A</i> in the sense of Van den Bergh (Trans Am Math Soc 360:5711–5799, 2008) is a bilinear map <span>\\(\\{\\!\\{-,-\\}\\!\\}\\)</span> from <span>\\(A\\times A\\)</span> to <span>\\(A^{\\otimes 2}\\)</span>, subject to certain conditions. Van den Bergh showed that any such bracket <span>\\(\\{\\!\\{-,-\\}\\!\\}\\)</span> induces Poisson structures on all algebras <span>\\(\\mathcal {O}(A,d)\\)</span>. We propose an analog of Van den Bergh’s construction, which produces Poisson structures on the coordinate rings of certain subspaces of the representation spaces <span>\\({\\text {Rep}}(A,d)\\)</span>. We call these subspaces the <i>involutive</i> representation spaces. They arise by imposing an additional symmetry condition on <span>\\({\\text {Rep}}(A,d)\\)</span>—just as the classical groups from the series B, C, D are obtained from the general linear groups (series A) as fixed point sets of involutive automorphisms.\n</p></div>","PeriodicalId":685,"journal":{"name":"Letters in Mathematical Physics","volume":null,"pages":null},"PeriodicalIF":1.3000,"publicationDate":"2024-02-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Letters in Mathematical Physics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s11005-024-01782-3","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, MATHEMATICAL","Score":null,"Total":0}
引用次数: 0
Abstract
Let \(\Bbbk \) be an algebraically closed field of characteristic 0 and A be a finitely generated associative \(\Bbbk \)-algebra, in general noncommutative. One assigns to A a sequence of commutative \(\Bbbk \)-algebras \(\mathcal {O}(A,d)\), \(d=1,2,3,\dots \), where \(\mathcal {O}(A,d)\) is the coordinate ring of the space \({\text {Rep}}(A,d)\) of d-dimensional representations of the algebra A. A double Poisson bracket on A in the sense of Van den Bergh (Trans Am Math Soc 360:5711–5799, 2008) is a bilinear map \(\{\!\{-,-\}\!\}\) from \(A\times A\) to \(A^{\otimes 2}\), subject to certain conditions. Van den Bergh showed that any such bracket \(\{\!\{-,-\}\!\}\) induces Poisson structures on all algebras \(\mathcal {O}(A,d)\). We propose an analog of Van den Bergh’s construction, which produces Poisson structures on the coordinate rings of certain subspaces of the representation spaces \({\text {Rep}}(A,d)\). We call these subspaces the involutive representation spaces. They arise by imposing an additional symmetry condition on \({\text {Rep}}(A,d)\)—just as the classical groups from the series B, C, D are obtained from the general linear groups (series A) as fixed point sets of involutive automorphisms.
期刊介绍:
The aim of Letters in Mathematical Physics is to attract the community''s attention on important and original developments in the area of mathematical physics and contemporary theoretical physics. The journal publishes letters and longer research articles, occasionally also articles containing topical reviews. We are committed to both fast publication and careful refereeing. In addition, the journal offers important contributions to modern mathematics in fields which have a potential physical application, and important developments in theoretical physics which have potential mathematical impact.