紧矩阵量子群G的余表示与其对偶量子群的关系

设 G=（A,△）为紧矩阵量子群,G为A的所有有限维光滑的、不可约余表示等价类的集合.本文通过（A,△）的一个余表示Vo构造了两个相互配对的集合,利用Hilbert C＊-模的理论证明它们分别为A和Baaj与Skandalis构造的量子群A,并且证明了对任意的α∈G,在A中都对应一个有限维投影算子Pα,满足 dim（α）=dim（pα）.     

紧矩阵量子群G的余表示与其对偶量子群(A)的关系

设 G=（A,△）为紧矩阵量子群,G为A的所有有限维光滑的、不可约余表示等价类的集合.本文通过（A,△）的一个余表示Vo构造了两个相互配对的集合,利用Hilbert C＊-模的理论证明它们分别为A和Baaj与Skandalis构造的量子群A,并且证明了对任意的α∈G,在A中都对应一个有限维投影算子Pα,满足 dim（α）=dim（pα）.     

紧量子群U_θ（2）的分类

本文将要证明紧量子群Uθ（2）的余表示完全由其无穷小生成元B0,B2,A0,A1与A2决定,其中θ为无理数.还将证明B0,B2与Aj交换,j=0,1,2,B0,A0,A1,A2生成了sl（2,C）的loop代数.而后我们将给出Uθ（2）的所有不可约表示,不同于古典酉群U（2）的表示,最后利用上述结论给出Uθ（2）的分类,这个分类相似于无理旋转代数Aθ的分类,同时刻画了Uθ（2）所有自同构.     

B型量子群的Kashiwara算子

利用一个带特殊自同构的A_2n-1型Dynkin箭图上的F-稳定表示,刻画了B型量子群的Kashiwara算子.同时指出邓、杜和张文章中的主要结果对于B₂型赋值箭图并不成立.     

IR量子群ν_q(sl(2 ) )的不可约表示(英文)

本文引进满足一定关系的六个元素生成的量子群 νq(sl(2 ) ) .证明了 νq(sl(2 ) )具有 PBW基且是无零因子环 .进而当 q不是单根时决定了νq(sl(2 ) )的有限维不可约束表示 .     

量子群u_q(sl(2))中理想的唯一分解

本文利用量子群uq(sl(2))的表示及其理想的生成子,证明了uq(sl(2))的任一非零理想在某种意义下可唯一分解为若干个素理想的乘积.由此得到理想的求根公式.     

量子群Uq(sl(2))中理想的唯一分解

本文利用量子群Uq(sl(2))的表示及其理想的生成子,证明了Uq(sl(2))的任一非零理想在某种意义下可唯一分解为若干个素理想的乘积.由此得到理想的求根公式.     

量子群Uq(D4)上不可约模的Grobner-Shirshov对

首先,利用量子群Uq (D4)的已知的Grobner-Shirshov基和Chibrikov的双自由模方法来计算量子群Uq(D4)上不可约模Vq(λ)的一个Grobner-Shirshov对,然后在Uq(D4)的适当形式U'q(D4)中取q=1得到D4型单李代数的泛包络代数U(D4)上不可约模V(λ)的一个Grobner-Shirshov对.     

Young表与Uq（osp（1｜2n））的晶体基

设Uq（osp（1｜2n））是对应Lie超代数osp（1｜2n）的量子包络超代数．利用满足一定条件的半标准Young表,给出有限维既约Uq（osp（1｜2n））模晶体图的实现．建立晶体图张量积分解的广义Littlewood—Richardson法则．     

Young表与$\textrm{U}_{q}(\mathrm{osp}(1|2n))$的晶体基

设 $U_q(\mathrm{osp}(1|2n))$是对应Lie超代数$\mathrm{osp}(1|2n)$的量子包络超代数. 利用满足一定条件的半标准Young表, 给出有限维既约$U_q(\mathrm{osp}(1|2n))$模晶体图的实现 . 建立晶体图张量积分解的广义Littlewood-Richardson法则.     

Tight Monomials for Type G 2 and A 3

The global crystal basis or canonical basis plays an important role in the theory of the quantum groups and their representations. The tight monomials are the simplest elements in the canonical basis. Based on Reineke, Deng, and Du's work, the tight monomials in quantized enveloping algebra of type G₂ and A₃ are completely determined in this article.     

Monomial Realization of Crystal Bases <Emphasis Type="Italic">B</Emphasis>(∞) for the Quantum Finite Algebras

In this paper, we give a new realization of the crystal basis B(∞) using modified Nakajima monomials for the quantum finite algebras. Moreover, as an application, we obtain the image of the Kashiwara embedding Ψ _ι from this realization of B(∞). Presented by Alain Verschoren.     

The Canonical Basis for the Quantum Group of Type B2

We use the Ringel-Hall algebra approach to study the canonical basis elements for the quantum group of type B₂ which are characterized in Xi [12]. However, our approach simplifies several computations there.     

The Role of Frame Force in Quantum Detection

A general method is given to solve tight frame optimization problems, borrowing notions from classical mechanics. In this article, we focus on a quantum detection problem, where the goal is to construct a tight frame that minimizes an error term, which in quantum physics has the interpretation of the probability of a detection error. The method converts the frame problem into a set of ordinary differential equations using concepts from classical mechanics and orthogonal group techniques. The minimum energy solutions of the differential equations are proven to correspond to the tight frames that minimize the error term. Because of this perspective, several numerical methods become available to compute the tight frames. Beyond the applications of quantum detection in quantum mechanics, solutions to this frame optimization problem can be viewed as a generalization of classical matched filtering solutions. As such, the methods we develop are a generalization of fundamental detection techniques in radar.      

Canonical Basis for Type A 4 (II)-Polynomial Elements in One Variable

ABSTRACT

All the 62 monomial elements in the canonical basis B of the quantized enveloping algebra for type A ₄ have been determined in Hu et al. (2003 Hu , Y. , Ye , J. , Yue , X. ( 2003 ). Canonical basis for type A ₄ (I)–Monomial elements . J. Algebra 263 : 228 – 245 . [CSA] [CROSSREF]  [Google Scholar]). According to Lusztig's idea (Lusztig, 1992 Lusztig , G. ( 1992 ). Introduction to quantized enveloping algebras . In: Tirao , J. , Wallach , N. , eds. New Developments in Lie Theory and Their Applications . Progress in Mathematics . Vol. 105 . Boston/Basel/Berlin : Birkhauser , pp. 49 – 65 . [Google Scholar]), the elements in the canonical basis B consist of monomials and linear combinations of monomials (for convenience, we call them polynomials). In this note, we compute all the 144 polynomial elements in one variable in the canonical basis B of the quantized enveloping algebra for type A ₄ based on our joint note Hu et al. (2003 Hu , Y. , Ye , J. , Yue , X. ( 2003 ). Canonical basis for type A ₄ (I)–Monomial elements . J. Algebra 263 : 228 – 245 . [CSA] [CROSSREF]  [Google Scholar]). We conjecture that there are other polynomial elements in two or three variables in the canonical basis B, which include independent variables and dependent variables. Moreover, it is conjectured that there are no polynomial elements in the canonical basis B with four or more variables.     

关于A_(n-1)型CHEVALLEY扩群■的唯一性

本文讨论[1]中留下的A_(n-1)型Chevalley群G≌SL_n(K)的扩群G的唯一性问题,得到群G在同构意义下至多有1/2φ(n)个。     

A 类量子群和 Hecke 代数的 Schur-Weyl 对偶

设Vm是量子群Uq（SLm)的标准表示,通过Hecke代数的作用,作者将Vm的张量积V^nm分解成了Uq(SLm)的不可约表示的直和,从而给出了Uq(SLm)与Hecke代数的H（q,n)Schur-Weyl对偶的完整证明,进一步得到,当q是实数时,在Hilbert空间H^n上,Uq(SL∞）和H（q,n)之间存在着Schur-Weyl对偶。     

Gr\"{o}bner-Shirshov Basis of Quantum Group of Type $\mathbb{D}_4$

The authors take all isomorphism classes of indecomposable representations as new generators, and obtain all skew-commutators between these generators by using the Ringel-Hall algebra method. Then they prove that the set of these skew-commutators is a Gröbner-Shirshov basis for quantum group of type \(\mathbb{D}_4\).