{"title":"双泊松括弧和非累加表示空间","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":"{\"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}","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
摘要
摘要 让 \(\Bbbk \) 是一个特征为 0 的代数闭域,A 是一个有限生成的关联 \(\Bbbk \) -代数,一般来说是非交换的。我们给 A 赋值一系列交换的 ( ( ( (Bbbk) ) )-代数)其中 \(\mathcal {O}(A,d)\) 是代数 A 的 d 维表示的空间 \({\text {Rep}}(A,d)\) 的坐标环。在范登贝格(Trans Am Math Soc 360:5711-5799, 2008)的意义上,A 上的双泊松括号是从\(A\times A\) 到\(A^{\times 2}\) 的双线性映射(\{\!Van den Bergh 证明了任何这样的括号 ({\!\{-,-\}\!!\})都会在所有的代数(\mathcal {O}(A,d)\) )上引起泊松结构。我们提出了 Van den Bergh 构建的类似方法,即在表示空间 \({\text {Rep}}(A,d)\) 的某些子空间的坐标环上产生泊松结构。我们称这些子空间为内卷表示空间。它们是通过在 \({\text {Rep}}(A,d)\) 上施加额外的对称条件而产生的--就像从一般线性群(系列 A)中得到的经典群(系列 B、C、D)是渐开自动形的定点集一样。
Double Poisson brackets and involutive representation spaces
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.