{"title":"A 型抛物线邻接作用的 nilfibre 的典型分量","authors":"","doi":"10.1007/s10801-023-01296-6","DOIUrl":null,"url":null,"abstract":"<h3>Abstract</h3> <p>This work is a continuation of [Y. Fittouhi and A. Joseph, Parabolic adjoint action, Weierstrass Sections and components of the nilfibre in type <em>A</em>]. Let <em>P</em> be a parabolic subgroup of an irreducible simple algebraic group <em>G</em>. Let <span> <span>\\(P'\\)</span> </span> be the derived group of <em>P</em>, and let <span> <span>\\({\\mathfrak {m}}\\)</span> </span> be the Lie algebra of the nilradical of <em>P</em>. A theorem of Richardson implies that the subalgebra <span> <span>\\({\\mathbb {C}}[{\\mathfrak {m}}]^{P'}\\)</span> </span>, spanned by the <em>P</em> semi-invariants in <span> <span>\\({\\mathbb {C}}[{\\mathfrak {m}}]\\)</span> </span>, is polynomial. A linear subvariety <span> <span>\\(e+V\\)</span> </span> of <span> <span>\\({\\mathfrak {m}}\\)</span> </span> is called a Weierstrass section for the action of <span> <span>\\(P'\\)</span> </span> on <span> <span>\\({\\mathfrak {m}}\\)</span> </span>, if the restriction map induces an isomorphism of <span> <span>\\({\\mathbb {C}}[{\\mathfrak {m}}]^{P'}\\)</span> </span> onto <span> <span>\\({\\mathbb {C}}[e+V]\\)</span> </span>. Thus, a Weierstrass section can exist only if the latter is polynomial, but even when this holds its existence is far from assured. Let <span> <span>\\({\\mathscr {N}}\\)</span> </span> be zero locus of the augmentation <span> <span>\\({\\mathbb {C}}[{\\mathfrak {m}}]^{P'}_+\\)</span> </span>. It is called the nilfibre relative to this action. Suppose <span> <span>\\(G=\\textrm{SL}(n,{\\mathbb {C}})\\)</span> </span>, and let <em>P</em> be a parabolic subgroup. In [Y. Fittouhi and A. Joseph, loc. cit.], the existence of a Weierstrass section <span> <span>\\(e+V\\)</span> </span> in <span> <span>\\({\\mathfrak {m}}\\)</span> </span> was established by a general combinatorial construction. Notably, <span> <span>\\(e \\in {\\mathscr {N}}\\)</span> </span> and is a sum of root vectors with linearly independent roots. The Weierstrass section <span> <span>\\(e+V\\)</span> </span> looks very different for different choices of parabolics but nevertheless has a uniform construction and exists in all cases. It is called the “canonical Weierstrass section”. Through [Y. Fittouhi and A. Joseph, loc. cit. Prop. 6.9.2, Cor. 6.9.8], there is always a “canonical” component <span> <span>\\({\\mathscr {N}}^e\\)</span> </span> of <span> <span>\\({\\mathscr {N}}\\)</span> </span> containing <em>e</em>. It was announced in [Y. Fittouhi and A. Joseph, loc. cit., Prop. 6.10.4] that one may augment <em>e</em> to an element <span> <span>\\(e_\\textrm{VS}\\)</span> </span> by adjoining root vectors. Then the linear span <span> <span>\\(E_\\textrm{VS}\\)</span> </span> of these root vectors lies in <span> <span>\\(\\mathscr {N}^e\\)</span> </span> and its closure is just <span> <span>\\({\\mathscr {N}}^e\\)</span> </span>. Yet, this same result shows that <span> <span>\\({\\mathscr {N}}^e\\)</span> </span> need <em>not</em> admit a dense <em>P</em> orbit [Y. Fittouhi and A. Joseph, loc. cit., Lemma 6.10.7]. For the above [Y. Fittouhi and A. Joseph, loc. cit., Theorem 6.10.3] was needed. However, this theorem was only verified in the special case needed to obtain the example showing that <span> <span>\\({\\mathscr {N}}^e\\)</span> </span> may fail to admit a dense <em>P</em> orbit. Here a general proof is given (Theorem 4.4.5). Finally, a map from compositions to the set of distinct non-negative integers is defined. Its image is shown to determine the canonical Weierstrass section. One may anticipate that the remaining components of <span> <span>\\({\\mathscr {N}}\\)</span> </span> can be similarly described. However, this is a long story and will be postponed for a subsequent paper. These results should form a template for general type.</p>","PeriodicalId":0,"journal":{"name":"","volume":null,"pages":null},"PeriodicalIF":0.0,"publicationDate":"2024-02-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The Canonical component of the nilfibre for parabolic adjoint action in type A\",\"authors\":\"\",\"doi\":\"10.1007/s10801-023-01296-6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<h3>Abstract</h3> <p>This work is a continuation of [Y. Fittouhi and A. Joseph, Parabolic adjoint action, Weierstrass Sections and components of the nilfibre in type <em>A</em>]. Let <em>P</em> be a parabolic subgroup of an irreducible simple algebraic group <em>G</em>. Let <span> <span>\\\\(P'\\\\)</span> </span> be the derived group of <em>P</em>, and let <span> <span>\\\\({\\\\mathfrak {m}}\\\\)</span> </span> be the Lie algebra of the nilradical of <em>P</em>. A theorem of Richardson implies that the subalgebra <span> <span>\\\\({\\\\mathbb {C}}[{\\\\mathfrak {m}}]^{P'}\\\\)</span> </span>, spanned by the <em>P</em> semi-invariants in <span> <span>\\\\({\\\\mathbb {C}}[{\\\\mathfrak {m}}]\\\\)</span> </span>, is polynomial. A linear subvariety <span> <span>\\\\(e+V\\\\)</span> </span> of <span> <span>\\\\({\\\\mathfrak {m}}\\\\)</span> </span> is called a Weierstrass section for the action of <span> <span>\\\\(P'\\\\)</span> </span> on <span> <span>\\\\({\\\\mathfrak {m}}\\\\)</span> </span>, if the restriction map induces an isomorphism of <span> <span>\\\\({\\\\mathbb {C}}[{\\\\mathfrak {m}}]^{P'}\\\\)</span> </span> onto <span> <span>\\\\({\\\\mathbb {C}}[e+V]\\\\)</span> </span>. Thus, a Weierstrass section can exist only if the latter is polynomial, but even when this holds its existence is far from assured. Let <span> <span>\\\\({\\\\mathscr {N}}\\\\)</span> </span> be zero locus of the augmentation <span> <span>\\\\({\\\\mathbb {C}}[{\\\\mathfrak {m}}]^{P'}_+\\\\)</span> </span>. It is called the nilfibre relative to this action. Suppose <span> <span>\\\\(G=\\\\textrm{SL}(n,{\\\\mathbb {C}})\\\\)</span> </span>, and let <em>P</em> be a parabolic subgroup. In [Y. Fittouhi and A. Joseph, loc. cit.], the existence of a Weierstrass section <span> <span>\\\\(e+V\\\\)</span> </span> in <span> <span>\\\\({\\\\mathfrak {m}}\\\\)</span> </span> was established by a general combinatorial construction. Notably, <span> <span>\\\\(e \\\\in {\\\\mathscr {N}}\\\\)</span> </span> and is a sum of root vectors with linearly independent roots. The Weierstrass section <span> <span>\\\\(e+V\\\\)</span> </span> looks very different for different choices of parabolics but nevertheless has a uniform construction and exists in all cases. It is called the “canonical Weierstrass section”. Through [Y. Fittouhi and A. Joseph, loc. cit. Prop. 6.9.2, Cor. 6.9.8], there is always a “canonical” component <span> <span>\\\\({\\\\mathscr {N}}^e\\\\)</span> </span> of <span> <span>\\\\({\\\\mathscr {N}}\\\\)</span> </span> containing <em>e</em>. It was announced in [Y. Fittouhi and A. Joseph, loc. cit., Prop. 6.10.4] that one may augment <em>e</em> to an element <span> <span>\\\\(e_\\\\textrm{VS}\\\\)</span> </span> by adjoining root vectors. Then the linear span <span> <span>\\\\(E_\\\\textrm{VS}\\\\)</span> </span> of these root vectors lies in <span> <span>\\\\(\\\\mathscr {N}^e\\\\)</span> </span> and its closure is just <span> <span>\\\\({\\\\mathscr {N}}^e\\\\)</span> </span>. Yet, this same result shows that <span> <span>\\\\({\\\\mathscr {N}}^e\\\\)</span> </span> need <em>not</em> admit a dense <em>P</em> orbit [Y. Fittouhi and A. Joseph, loc. cit., Lemma 6.10.7]. For the above [Y. Fittouhi and A. Joseph, loc. cit., Theorem 6.10.3] was needed. However, this theorem was only verified in the special case needed to obtain the example showing that <span> <span>\\\\({\\\\mathscr {N}}^e\\\\)</span> </span> may fail to admit a dense <em>P</em> orbit. Here a general proof is given (Theorem 4.4.5). Finally, a map from compositions to the set of distinct non-negative integers is defined. Its image is shown to determine the canonical Weierstrass section. One may anticipate that the remaining components of <span> <span>\\\\({\\\\mathscr {N}}\\\\)</span> </span> can be similarly described. However, this is a long story and will be postponed for a subsequent paper. These results should form a template for general type.</p>\",\"PeriodicalId\":0,\"journal\":{\"name\":\"\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0,\"publicationDate\":\"2024-02-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"\",\"FirstCategoryId\":\"100\",\"ListUrlMain\":\"https://doi.org/10.1007/s10801-023-01296-6\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"","FirstCategoryId":"100","ListUrlMain":"https://doi.org/10.1007/s10801-023-01296-6","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
摘要 本文是 [Y. Fittouhi 和 A. Joseph, Parabolic adjoint action, Weierstrass Sections and components in type A] 的继续。Fittouhi and A. Joseph, Parabolic adjoint action, Weierstrass Sections and components of the nilfibre in type A].设 P 是不可还原简单代数群 G 的抛物线子群。让 \(P'\) 是 P 的导出群,让 \({\mathfrak {m}}\) 是 P 的 nilradical 的李代数。理查森(Richardson)的一个定理意味着子代数 \({\mathbb {C}}[{\mathfrak {m}}]^{P'}\) ,由 \({\mathbb {C}}[{\mathfrak {m}}]\) 中的 P 半变量所跨,是多项式的。P'\)对\({\mathfrak {m}}\)的作用的一个线性子变量\(e+V\)被称为魏尔斯特拉斯截面、如果限制映射引起了 \({\mathbb {C}}[{\mathfrak {m}}]^{P'}\) 到 \({\mathbb {C}}[e+V]\) 的同构。因此,魏尔斯特拉斯截面只有在后者是多项式的情况下才会存在,但即使这一点成立,它的存在也远未得到保证。让 \({\mathscr {N}}\) 成为增强 \({\mathbb {C}}[{\mathfrak {m}}]^{P'}_+\) 的零点。相对于这个动作,它被称为无纤维。假设 \(G=\textrm{SL}(n,{\mathbb {C}})\),并让 P 是一个抛物线子群。在[Y. Fittouhi and A. Joseph, loc. cit.]中,通过一个一般的组合构造证明了在\({mathfrak {m}\}) 中存在一个魏尔斯特拉斯截面\(e+V\)。值得注意的是\(e \in {\mathscr {N}}\) 是具有线性独立根的根向量之和。对于抛物线的不同选择,魏尔斯特拉斯截面(e+V)看起来非常不同,但它有统一的构造,并且在所有情况下都存在。它被称为 "典型魏尔斯特拉斯截面"。通过[Y. Fittouhi and A. Joseph, loc. cit. Prop. 6.9.2, Cor. 6.9.8],\({\mathscr {N}}^e\) 总是存在一个包含 e 的 "规范 "部分 \({\mathscr {N}}^e\) 、Prop. 6.10.4] 中宣布,我们可以通过邻接根向量将 e 增为元素 \(e_textrm{VS}/)。那么这些根向量的线性跨度 \(E_textrm{VS}\) 位于 \(\mathscr {N}^e\) 中,它的闭包就是 \({\mathscr {N}}^e\) 。然而,同样的结果表明,\({\mathscr {N}^e\) 不一定要有密集的 P 轨道[Y. Fittouhi and A. Joseph, loc. cit., Lemma 6.10.7]。为此,我们需要[Y. Fittouhi and A. Joseph, loc. cit., Theorem 6.10.3]。然而,这个定理只在特例中得到了验证,这个特例表明 \({\mathscr {N}}^e\) 可能无法接纳密集的 P 轨道。这里给出了一般证明(定理 4.4.5)。最后,定义了一个从构成到不同非负整数集合的映射。它的图象被证明可以确定典范魏尔斯特拉斯截面。我们可以预料到 \({\mathscr {N}}\) 的其余成分也可以得到类似的描述。然而,这是一个很长的故事,将推迟到以后的论文中讨论。这些结果应该成为一般类型的模板。
The Canonical component of the nilfibre for parabolic adjoint action in type A
Abstract
This work is a continuation of [Y. Fittouhi and A. Joseph, Parabolic adjoint action, Weierstrass Sections and components of the nilfibre in type A]. Let P be a parabolic subgroup of an irreducible simple algebraic group G. Let \(P'\) be the derived group of P, and let \({\mathfrak {m}}\) be the Lie algebra of the nilradical of P. A theorem of Richardson implies that the subalgebra \({\mathbb {C}}[{\mathfrak {m}}]^{P'}\), spanned by the P semi-invariants in \({\mathbb {C}}[{\mathfrak {m}}]\), is polynomial. A linear subvariety \(e+V\) of \({\mathfrak {m}}\) is called a Weierstrass section for the action of \(P'\) on \({\mathfrak {m}}\), if the restriction map induces an isomorphism of \({\mathbb {C}}[{\mathfrak {m}}]^{P'}\) onto \({\mathbb {C}}[e+V]\). Thus, a Weierstrass section can exist only if the latter is polynomial, but even when this holds its existence is far from assured. Let \({\mathscr {N}}\) be zero locus of the augmentation \({\mathbb {C}}[{\mathfrak {m}}]^{P'}_+\). It is called the nilfibre relative to this action. Suppose \(G=\textrm{SL}(n,{\mathbb {C}})\), and let P be a parabolic subgroup. In [Y. Fittouhi and A. Joseph, loc. cit.], the existence of a Weierstrass section \(e+V\) in \({\mathfrak {m}}\) was established by a general combinatorial construction. Notably, \(e \in {\mathscr {N}}\) and is a sum of root vectors with linearly independent roots. The Weierstrass section \(e+V\) looks very different for different choices of parabolics but nevertheless has a uniform construction and exists in all cases. It is called the “canonical Weierstrass section”. Through [Y. Fittouhi and A. Joseph, loc. cit. Prop. 6.9.2, Cor. 6.9.8], there is always a “canonical” component \({\mathscr {N}}^e\) of \({\mathscr {N}}\) containing e. It was announced in [Y. Fittouhi and A. Joseph, loc. cit., Prop. 6.10.4] that one may augment e to an element \(e_\textrm{VS}\) by adjoining root vectors. Then the linear span \(E_\textrm{VS}\) of these root vectors lies in \(\mathscr {N}^e\) and its closure is just \({\mathscr {N}}^e\). Yet, this same result shows that \({\mathscr {N}}^e\) need not admit a dense P orbit [Y. Fittouhi and A. Joseph, loc. cit., Lemma 6.10.7]. For the above [Y. Fittouhi and A. Joseph, loc. cit., Theorem 6.10.3] was needed. However, this theorem was only verified in the special case needed to obtain the example showing that \({\mathscr {N}}^e\) may fail to admit a dense P orbit. Here a general proof is given (Theorem 4.4.5). Finally, a map from compositions to the set of distinct non-negative integers is defined. Its image is shown to determine the canonical Weierstrass section. One may anticipate that the remaining components of \({\mathscr {N}}\) can be similarly described. However, this is a long story and will be postponed for a subsequent paper. These results should form a template for general type.