Explicit Construction of Exact Unitary Designs

Total Page:16

File Type:pdf, Size:1020Kb

Load more

Explicit construction of exact unitary designs Eiichi Bannai ∗ Yoshifumi Nakata † Takayuki Okuda ‡ Da Zhao § September 24, 2020 Abstract The purpose of this paper is to give explicit constructions of unitary t- designs in the unitary group U(d) for all t and d. It seems that the explicit constructions were so far known only for very special cases. Here explicit construction means that the entries of the unitary matrices are given by the values of elementary functions at the root of some given polynomials. We will discuss what are the best such unitary 4-designs in U(4) obtained by these methods. Indeed we give an inductive construction of designs on compact groups by using Gelfand pairs (G, K). Note that (U(n), U(m) × U(n − m)) is a Gelfand pair. By using the zonal spherical functions for (G, K), we can construct designs on G from designs on K. We remark that our proofs use the representation theory of compact groups crucially. We also remark that this method can be applied to the orthogonal groups O(d), and thus provides another explicit construction d 1 of spherical t-designs on the d dimensional sphere S − by the induction on d. 1 Introduction The aim of design theory is to approximate a space M by a good finite subset X. arXiv:2009.11170v1 [math.CO] 23 Sep 2020 There have been numerous studies on spherical designs[17] and combinatorial designs[14]. The sphere is a canonical continuous space while the combinatorial V design is in the discrete space M = k of k-subsets of V . The concept of ∗Professor Emeritus of Kyushu University, Fukuoka, Japan. Postal Address: Asagaya- minami 3-2-33, Suginami-ku, Tokyo 166-0004, Japan. [email protected] †Photon Science Center, Graduate School of Engineering, The University of Tokyo, Bunkyo-ku, Tokyo 113-8656, Japan. JST, PRESTO, 4-1-8 Honcho, Kawaguchi, Saitama, 332-0012, Japan. [email protected] ‡Department of Mathematics, Hiroshima University, 1-3-1 Kagamiyama, Higashihiroshima, 739-8526, Japan. [email protected] §School of Mathematical Sciences, Shanghai Jiao Tong University, 800 Dongchuan Road, Minhang District, Shanghai 200240, China. [email protected] 1 combinatorial design was generalized to designs on Q-polynomial association schemes[16]. Other continuous spaces such as projective space, Grassmannian space[1, 2, 38] have been considered as well. In this paper we focus on the construction of unitary designs, which is designs on the unitary group. There is an increasing demand for unitary designs in quantum information science that aims to realize information processing based on quantum mechan- ics, where protocols are described by unitary transformations. Physically im- plementing unitary transformations is the key to realize information processing in quantum information science. A unitary transformation chosen uniformly at random from the whole unitary group is of particular importance since it is used in many protocols, such as benchmarking quantum devices [18, 30], characteriz- ing quantum systems [31, 36, 40], improving computational complexity [11], and transmitting information [27]. However, the resources available in experiments are quite limited and so, it is in general hard to experimentally implement the uniformly random unitary transformation. Thus, mimicking the whole unitary group by unitary designs is attracting much attention. While numerous constructions of unitary 2-designs are known [37, 13, 28, 21, 25, 34], less is known about unitary t-designs for t 3 [10, 23, 24, 26, 33]. Most of them are approximate ones. Hence, finding explicit≥ constructions of exact unitary t-designs on U(d) is highly desired, which will lead to more accurate realizations of quantum information protocols. Some finite subgroups of the unitary group are unitary designs of small strength[7, 22, 39]. The Clifford groups on U(2n) for any n N are exact unitary 3-designs[44, 48, 49]. An exact unitary 4-design on U(4) is∈ constructed in [6]. The main purpose of this paper is to provide inductive constructions of exact unitary t-design on U(d) for arbitrary strength t and dimension d. The method can be applied to orthogonal groups as well. As a by-product we have constructions for complex spherical designs and real spherical designs. The existence of spherical designs were proved by Seymour-Zaslavsky[41]. Bondarenko-Radchenko-Viazovsk[9] showed that there exist spherical t-designs d d on S of size at least cdt for some fixed constant cd with t tending to infin- ity. This lower bound is asymptotically best possible order of magnitude. The asymptotically best lower bound for fixed strength t with d tending to infinity is yet unknown. The explicit construction of spherical designs is relatively in- volved. Rabau-Bajnok[35] and Wagner[43] constructed spherical t-designs from interval t-designs with Gegenbauer weight. Cui-Xia-Xiang[15] showed the ex- istence of spherical designs over Q(√p) where p is a prime number. Later Xiang[47] obtained explicit spherical designs. The readers can find surveys on spherical designs in [3, 4]. Let us now define unitary designs. There are several equivalent definitions of unitary t-designs. Definition 1.1 ([39, pp. 14-15]). Let X be a finite subset X of U(d). The following are equivalent. 1. X is a unitary t-design. 2 2. 1 U ⊗t (U †)⊗t = U ⊗t (U †)⊗t dU. |X| U∈X ⊗ U(d) ⊗ 3. 1 P f(U)= f(UR) dU for every f Hom(U(d),t,t), the space |X| U∈X U(d) ∈ of polynomials of homogeneous degree t in entries of U and of homogeneous P R † degree t in the entries of U . Representation theory is used extensively in our construction. There is an- other equivalent definition of unitary t-designs by irreducible representations of U(d), which is quite useful for our purpose. The irreducible representations of unitary group are characterized by the highest weight. Theorem 1.1 ([12, Theorem 25.5]). The irreducible representations of unitary group U(n) are indexed by non-increasing integer sequence λ = (λ1, λ2,...,λn) of length n. + − We denote by λ the sum of positive terms in λ1, λ2,...,λn and by λ the absolute value of sum of negative terms in λ1, λ2,...,λn. And we define λ = λ+ λ−. The following two collections of irreducible representations are used| | to characterize− unitary design. s,t := λ : λ λ λ , λ+ s, λ− t . n { 1 ≥ 2 ≥···≥ n ≤ ≤ } t := λ : λ λ λ , λ+ = λ− t t,t. n { 1 ≥ 2 ≥···≥ n ≤ }⊂ n Theorem 1.2 ([6, Theorem 6]). A finite subset X U(d) is a unitary t-design if and only if ⊂ 1 ρ (U)= ρ (U) dU. (1) X λ λ U X U(d) | | X∈ Z for every irreducible representation ρ where λ t . λ ∈ n t t,t Due to the inductive nature of our construction, we will replace n by n . We will also adopt the relaxation from set to multi-set for technical reasons. Definition 1.2. Let X be a finite multi-set on U(d). The following are equiv- alent. 1. X is a strong unitary t-design on U(d). 1 ⊗r † ⊗s ⊗r † ⊗s 2. |X| U∈X U (U ) = U(d) U (U ) dU for every integers 0 r, s t. ⊗ ⊗ ≤ P≤ R 3. 1 f(U)= f(U) dU for every f Hom(U(d),r,s), the space |X| U∈X U(d) ∈ of polynomials of homogeneous degree r in entries of U and of homoge- P R neous degree s in the entries of U †, for every integers 0 r, s t. ≤ ≤ 4. 1 ρ (U)= ρ (U) dU for every λ t,t. |X| U∈X λ U(d) λ ∈ n This paperP shows the followingR theorem. 3 Theorem. Strong unitary t-designs on U(n) can be constructed from strong unitary t-designs on U(m) and strong unitary t-designs on U(n m) using the zeroes of zonal spherical functions of the complex Grassmannian− . Gm,n The paper is organized as follows. In Sections 2 to 4 the notation for multi- sets, representations and Haar measure are set up. In Section 5 we introduce Gelfand pairs and zonal spherical functions. The central object in this paper, designs on compact groups, are given in Section 6. We explain our inductive construction in Section 7. In Section 9 we compare different constructions of unitary 4-designs on U(4). We briefly mention how our method gives spherical designs as a by-product in Section 10. And finally in Section 11 we discuss the relation between designs in this paper and those in classic design theory. The Appendix include the zonal polynomials together with their zeroes. 2 finite multi-sets on groups Let G be a group. We use the terminology of “non-empty finite multi-sets X on G” in the following sense: Let N Z . Each S -orbit in GN is ∈ ≥1 N said to be an N-point multi-set on G, where GN denotes the direct product N of N-copies of G and SN the symmetric group of order N acting on G as permutations of coordinates. For the simplicity, the S -orbit of (x ,...,x ) N 1 N ∈ GN will be denoted by x ,...,x . Note that x , x ,...,x = { 1 N }mult { 1 2 N }mult 6 x2,...,xN mult even if x1 = x2. { We also} use the following notation: For each N-point multi-set X = x1,...,xN mult on G, we put X := N • and { } | | N ρ(x) := ρ(xi) x X i=1 X∈ X for each map ρ : G W where W is an Abelian group.
Recommended publications
  • Physics.Hist-Ph] 15 May 2018 Meitl,Fo Hsadsadr Nepeainlprinciples

    Physics.Hist-Ph] 15 May 2018 Meitl,Fo Hsadsadr Nepeainlprinciples

    Why Be Regular?, Part I Benjamin Feintzeig Department of Philosophy University of Washington JB (Le)Manchak, Sarita Rosenstock, James Owen Weatherall Department of Logic and Philosophy of Science University of California, Irvine Abstract We provide a novel perspective on “regularity” as a property of representations of the Weyl algebra. We first critique a proposal by Halvorson [2004, “Complementarity of representa- tions in quantum mechanics”, Studies in History and Philosophy of Modern Physics 35(1), pp. 45–56], who argues that the non-regular “position” and “momentum” representations of the Weyl algebra demonstrate that a quantum mechanical particle can have definite values for position or momentum, contrary to a widespread view. We show that there are obstacles to such an intepretation of non-regular representations. In Part II, we propose a justification for focusing on regular representations, pace Halvorson, by drawing on algebraic methods. 1. Introduction It is standard dogma that, according to quantum mechanics, a particle does not, and indeed cannot, have a precise value for its position or for its momentum. The reason is that in the standard Hilbert space representation for a free particle—the so-called Schr¨odinger Representation of the Weyl form of the canonical commutation relations (CCRs)—there arXiv:1805.05568v1 [physics.hist-ph] 15 May 2018 are no eigenstates for the position and momentum magnitudes, P and Q; the claim follows immediately, from this and standard interpretational principles.1 Email addresses: [email protected] (Benjamin Feintzeig), [email protected] (JB (Le)Manchak), [email protected] (Sarita Rosenstock), [email protected] (James Owen Weatherall) 1Namely, the Eigenstate–Eigenvalue link, according to which a system has an exact value of a given property if and only if its state is an eigenstate of the operator associated with that property.
  • Fourier Analysis Using Representation Theory

    Fourier Analysis Using Representation Theory

    FOURIER ANALYSIS USING REPRESENTATION THEORY NEEL PATEL Abstract. In this paper, it is our goal to develop the concept of Fourier transforms by using Representation Theory. We begin by laying basic def- initions that will help us understand the definition of a representation of a group. Then, we define representations and provide useful definitions and the- orems. We study representations and key theorems about representations such as Schur's Lemma. In addition, we develop the notions of irreducible repre- senations, *-representations, and equivalence classes of representations. After doing so, we develop the concept of matrix realizations of irreducible represen- ations. This concept will help us come up with a few theorems that lead up to our study of the Fourier transform. We will develop the definition of a Fourier transform and provide a few observations about the Fourier transform. Contents 1. Essential Definitions 1 2. Group Representations 3 3. Tensor Products 7 4. Matrix Realizations of Representations 8 5. Fourier Analysis 11 Acknowledgments 12 References 12 1. Essential Definitions Definition 1.1. An internal law of composition on a set R is a product map P : R × R ! R Definition 1.2. A group G, is a set with an internal law of composition such that: (i) P is associative. i.e. P (x; P (y; z)) = P (P (x; y); z) (ii) 9 an identity; e; 3 if x 2 G; then P (x; e) = P (e; x) = x (iii) 9 inverses 8x 2 G, denoted by x−1, 3 P (x; x−1) = P (x−1; x) = e: Let it be noted that we shorthand P (x; y) as xy.
  • Factorization of Unitary Representations of Adele Groups Paul Garrett Garrett@Math.Umn.Edu

    Factorization of Unitary Representations of Adele Groups Paul Garrett [email protected]

    (February 19, 2005) Factorization of unitary representations of adele groups Paul Garrett [email protected] http://www.math.umn.edu/˜garrett/ The result sketched here is of fundamental importance in the ‘modern’ theory of automorphic forms and L-functions. What it amounts to is proof that representation theory is in principle relevant to study of automorphic forms and L-function. The goal here is to get to a coherent statement of the basic factorization theorem for irreducible unitary representations of reductive linear adele groups, starting from very minimal prerequisites. Thus, the writing is discursive and explanatory. All necessary background definitions are given. There are no proofs. Along the way, many basic concepts of wider importance are illustrated, as well. One disclaimer is necessary: while in principle this factorization result makes it clear that representation theory is relevant to study of automorphic forms and L-functions, in practice there are other things necessary. In effect, one needs to know that the representation theory of reductive linear p-adic groups is tractable, so that conversion of other issues into representation theory is a change for the better. Thus, beyond the material here, one will need to know (at least) the basic properties of spherical and unramified principal series representations of reductive linear groups over local fields. The fact that in some sense there is just one irreducible representation of a reductive linear p-adic group will have to be pursued later. References and historical notes
  • 23 Infinite Dimensional Unitary Representations

    23 Infinite Dimensional Unitary Representations

    23 Infinite dimensional unitary representations Last lecture, we found the finite dimensional (non-unitary) representations of SL2(R). 23.1 Background about infinite dimensional representa- tions (of a Lie group G) What is an infinite dimensional representation? 1st guess Banach space acted on by G? This is no good for the following reasons: Look at the action of G on the functions on G (by left translation). We could use L2 functions, or L1 or Lp. These are completely different Banach spaces, but they are essentially the same representation. 2nd guess Hilbert space acted on by G? This is sort of okay. The problem is that finite dimensional representations of SL2(R) are NOT Hilbert space representations, so we are throwing away some interesting representations. Solution (Harish-Chandra) Take g to be the Lie algebra of G, and let K be the maximal compact subgroup. If V is an infinite dimensional representation of G, there is no reason why g should act on V . The simplest example fails. Let R act on L2(R) by left translation. Then d d 2 R d the Lie algebra is generated by dx (or i dx ) acting on L ( ), but dx of an L2 function is not in L2 in general. Let V be a Hilbert space. Set Vω to be the K-finite vectors of V , which are the vectors contained in a finite dimensional representation of K. The point is that K is compact, so V splits into a Hilbert space direct sum finite dimensional representations of K, at least if V is a Hilbert space.
  • Lecture 1: Group C*-Algebras and Actions of Finite Groups on C*-Algebras 11–29 July 2016

    Lecture 1: Group C*-Algebras and Actions of Finite Groups on C*-Algebras 11–29 July 2016

    The Second Summer School on Operator Algebras and Noncommutative Geometry 2016 East China Normal University, Shanghai Lecture 1: Group C*-algebras and Actions of Finite Groups on C*-Algebras 11{29 July 2016 Lecture 1 (11 July 2016): Group C*-algebras and Actions of Finite N. Christopher Phillips Groups on C*-Algebras Lecture 2 (13 July 2016): Introduction to Crossed Products and More University of Oregon Examples of Actions. Lecture 3 (15 July 2016): Crossed Products by Finite Groups; the 11 July 2016 Rokhlin Property. Lecture 4 (18 July 2016): Crossed Products by Actions with the Rokhlin Property. Lecture 5 (19 July 2016): Crossed Products of Tracially AF Algebras by Actions with the Tracial Rokhlin Property. Lecture 6 (20 July 2016): Applications and Problems. N. C. Phillips (U of Oregon) Group C*-Algebras, Actions of Finite Groups 11 July 2016 1 / 28 N. C. Phillips (U of Oregon) Group C*-Algebras, Actions of Finite Groups 11 July 2016 2 / 28 A rough outline of all six lectures General motivation The material to be described is part of the structure and classification The beginning: The C*-algebra of a group. theory for simple nuclear C*-algebras (the Elliott program). More Actions of finite groups on C*-algebras and examples. specifically, it is about proving that C*-algebras which appear in other Crossed products by actions of finite groups: elementary theory. parts of the theory (in these lectures, certain kinds of crossed product C*-algebras) satisfy the hypotheses of known classification theorems. More examples of actions. Crossed products by actions of finite groups: Some examples.
  • CHAPTER 2 Representations of Finite Groups in This Chapter We Consider

    CHAPTER 2 Representations of Finite Groups in This Chapter We Consider

    CHAPTER 2 Representations of Finite Groups In this chapter we consider only finite-dimensional representations. 2.1. Unitarity, complete reducibility, orthogonality relations Theorem 1. A representation of a finite group is unitary. c Proof. Let (π, V ) be a (finite- dimensional) representation of a finite group G = { g1, g2, . gn }. Let h·, ·i1 be any inner product on V . Set n X hv, wi = hπ(gj)v, π(gj)wi1, v, w ∈ V. j=1 Then it is clear from the definition that hπ(g)v, π(g)wi = hv, wi, v, w ∈ V, g ∈ G. Pn Note that if v ∈ V , then hv, vi = j=1hπ(gj)v, π(gj)vi1 and if v 6= 0, then π(gj)v 6= 0 for all j implies hπ(gj)v, π(gj)vi1 > 0 for all j. Hence v 6= 0 implies hv, vi > 0. The other properties of inner product are easy to verify for h·, ·i, using the fact that h·, ·i1 is an inner product, and each π(gj) is linear. The details are left as an exercise. qed The following is an immediate consequence of Theorem 1 and a result from Chapter I stating that a finite-dimensional unitary representation is completely reducible. Theorem 2. A representation of a finite group is completely reducible. Example. Let G be a finite group acting on a finite set X. Let V be a complex vector space having a basis { vx1 , . , vxm } indexed by the elements x1, . , xm of X. If g ∈ G, let π(g) be the operator sending vxj to vg·xj , 1 ≤ j ≤ m.
  • On a Representation of the Group GL (K; R) and Its Spherical Functions

    On a Representation of the Group GL (K; R) and Its Spherical Functions

    Mem Fac ut & scl Shrmane Univ., Nat. Sci. 4, pp. Io 06 March 15 1971 On a RepreSentation of The Group GL (k; R) and ItS Spherical FunctionS Yasuhiro ASOo (Department of Mathematlcs shlmane Unrversity, Mat**ue, Japan) (Received October 12, 1970) In 1961, A. T. James [1] introduced the zonal polynomial of real positive definite matrix and he described some properties and a method of calculation of it. Lately, he [2] also showed that it is ' an eigenfunction of the Laplace-~eltrami operator. The '_onal polynomial plays significant roles in di-~*tribution problem** of eigenvalues related to the normal multivariate distri.bution [3]. In the present paper, we will describe a representation of the group G'L (k ; R) and its spherical functions guided by N. J. Vilenkin [4]. Our assumptions I and 2 in the following may be satisfied with zonal polynomials. We also give a deLinition of (zonal) spherical function of the group GL (k ; R) guided by K. Maurin [5] and we show that our zonal spherical function is in agreement with the latter definition. S I . Definitiola of spherical functions and son~_e properties related to the representation A(2f) (g) of th:e group GL (k ; R) Let { {g}(2)}(f), g E GL (k ; R) be a representation of the group GL (k ; R) on the space Vf of hornogeneous polynomials of degree f of the matrix ~;t ~ S, where ~;t is the space of real positive definite matrices of order k. Owing to Thrall [6]-Hua [71 's result, the representation space space Vf is completely decomposable mto rrreducrble mvanant subspaces V(f) on which representation A(2f,,.
  • Expander Graphs and Kazhdan's Property (T) Giles Gardam

    Expander Graphs and Kazhdan's Property (T) Giles Gardam

    Expander Graphs and Kazhdan's Property (T) Giles Gardam An essay submitted in partial fulfillment of the requirements for the degree of B.Sc. (Honours) Pure Mathematics University of Sydney October 2012 Contents Introduction ........................................................................ iv Acknowledgements ................................................................. vi Chapter 1. Expander Graphs.................................................... 1 1.1. Graph Theory Background . 1 1.2. Introduction to Expander Graphs . 5 1.3. Diameter in Expanders. 8 1.4. Alternative Definitions of Expansion . 10 1.5. Existence of Expanders . 13 1.6. Cayley Graphs . 14 1.7. Some Negative Results for Cayley Graph Expansion. 15 1.8. Expansion in SL(2; Z=pZ)..................................................... 17 Chapter 2. Random Walks on Expanders ...................................... 19 2.1. Random Walks and the Graph Spectrum . 19 2.2. Spectral Expansion . 20 2.3. Efficient Error Reduction for RP .............................................. 23 Chapter 3. Kazhdan's Property (T) ............................................ 27 3.1. Unitary Representations of Locally Compact Groups . 27 3.2. Property (T). 33 3.3. Compact Groups Have Property (T) . 37 3.4. Kazhdan Sets and Generation . 41 3.5. Lattices and Property (T). 44 3.6. Some Non-compact Kazhdan Groups . 46 Chapter 4. Constructions of Expanders ........................................ 51 4.1. Kazhdan Expanders. 51 4.2. Margulis's Construction of Expanders . 54 Appendix A. Asymptotic Representations
  • Hyperspherical Functions and Harmonic Analysis on the Lorentz

    Hyperspherical Functions and Harmonic Analysis on the Lorentz

    Hyperspherical Functions and Harmonic Analysis on the Lorentz Group V. V. Varlamov Department of Mathematics, Siberia State University of Industry, Kirova 42, Novokuznetsk 654007, Russia. Abstract Matrix elements of spinor and principal series representations of the Lorentz group are studied in the basis of complex angular momentum (helicity basis). It is shown that matrix elements are expressed via hyperspherical functions (relativistic spherical functions). In essence, the hyperspherical functions present itself a four-dimensional (with respect to a pseudo-euclidean metrics of Minkowski spacetime) generalization of the usual three-dimensional spherical functions. An explicit form of the hyperspher- ical functions is given. The hypespherical functions of the spinor representations are represented by a product of generalized spherical functions and Jacobi functions. It is shown that zonal hyperspherical functions are expressed via the Appell functions. The associated hyperspherical functions are defined as the functions on a two-dimensional complex sphere. Integral representations, addition theorems, symmetry and recur- rence relations for hyperspherical functions are given. In case of the principal and supplementary series representations of the Lorentz group, the matrix elements are ex- pressed via the functions represented by a product of spherical and conical functions. The hyperspherical functions of the principal series representations allow one to apply methods of harmonic analysis on the Lorentz group. Different forms of expansions of square integrable functions on the Lorentz group are studied. By way of example, an expansion of the wave function, representing the Dirac field (1/2, 0) (0, 1/2), is given. ⊕ arXiv:math-ph/0308039v2 21 May 2004 1 Introduction Numerous applications of three-dimensional spherical functions in different areas of mathe- matical and theoretical physics are well known.
  • Stone - Von Neumann Theorem

    Stone - Von Neumann Theorem

    (April 22, 2015) Stone - von Neumann theorem Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ The bibliography indicates the origins of these issues in proving uniqueness, up to isomorphism, of the model for the commutation rules of quantum mechanics. As Mackey and Weil observed, some form of the argument succeeds in quite general circumstances. The argument here is an amalgam and adaptation of those in sources in the bibliography. The proof here applies nearly verbatim, with suitable adjustment of the notion of Schwartz space, to Heisenberg groups over other local fields in place of R. Fix a finite-dimensional R-vectorspace V with non-degenerate alternating form h; i. The corresponding Heisenberg group has Lie algebra h = V ⊕ R, with Lie bracket 0 0 0 [v + z; v + z ] = hv; v i 2 R ≈ f0g ⊕ R ⊂ V ⊕ R Exponentiating to the Lie group H, the group operation is hv; v0i exp(v + z) · exp(v0 + z0) = exp v + v0 + z + z0 + 2 This is explained by literal matrix exponentiation: for example, with v = (x; y) 2 R2, 0 1 0 xy 1 0 x z 1 x z + 2 exp(v + z) = exp @ 0 0 y A = @ 0 1 y A (with v = (x; y)) 0 0 0 0 0 1 We use Lie algebra coordinates on H, often suppressing the exponential on abelian subgroups, but reinstating an explicit exponential notation when necessary to avoid confusion. [0.0.1] Theorem: (Stone-vonNeumann) For fixed non-trivial unitary central character, up to isomorphism there is a unique irreducible unitary representation of the Heisenberg group with that central character.
  • Unitary Representations of Topological Groups

    Unitary Representations of Topological Groups

    (July 28, 2014) Unitary representations of topological groups Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ We develop basic properties of unitary Hilbert space representations of topological groups. The groups G are locally-compact, Hausdorff, and countably based. This is a slight revision of my handwritten 1992 notes, which were greatly influenced by [Robert 1983]. Nothing here is new, apart from details of presentation. See the brief notes on chronology at the end. One purpose is to isolate techniques and results in representation theory which do not depend upon additional structure of the groups. Much can be done in the representation theory of compact groups without anything more than the compactness. Similarly, the discrete decomposition of L2(ΓnG) for compact quotients ΓnG depends upon nothing more than compactness. Schur orthogonality and inner product relations can be proven for discrete series representations inside regular representations can be discussed without further hypotheses. The purely topological treatment of compact groups shows a degree of commonality between subsequent treatments of Lie groups and of p-adic groups, whose rich details might otherwise obscure the simplicity of some of their properties. We briefly review Haar measure, and prove the some basic things about invariant measures on quotients HnG, where this notation refers to a quotient on the left, consisting of cosets Hg. We briefly consider Gelfand-Pettis integrals for continuous compactly-supported vector valued functions with values in Hilbert spaces. We emphasize discretely occurring representations, neglecting (continuous) Hilbert integrals of representa- tions. Treatment of these discrete series more than suffices for compact groups.
  • Discretely Decomposable Restrictions of $(\Mathfrak {G}, K) $-Modules For

    Discretely Decomposable Restrictions of $(\Mathfrak {G}, K) $-Modules For

    DISCRETELY DECOMPOSABLE RESTRICTIONS OF (g,K)-MODULES FOR KLEIN FOUR SYMMETRIC PAIRS OF EXCEPTIONAL LIE GROUPS OF HERMITIAN TYPE HAIAN HE Abstract. Let (G,GΓ) be a Klein four symmetric pair. The author wants to classify all the Klein four symmetric pairs (G,GΓ) such that there exists at least one nontrivial unitarizable simple (g,K)-module πK that is discretely decomposable as a (gΓ,KΓ)-module. In this article, three assumptions will be made. Firstly, G is an exceptional Lie group of Hermitian Γ type, i.e., G = E6(−14) or E7(−25). Secondly, G is noncompact. Thirdly, there exists an element σ ∈ Γ corresponding to a symmetric pair of anti-holomorphic type such that πK is discretely decomposable as a (gσ ,Kσ)-module. 1. Introduction Let G be a noncompact simple Lie group, and G′ a reductive subgroup of G. Write g and g′ for the complexified Lie algebras of G and G′ respectively. Take a maximal compact subgroup K of G such that K′ := K G′ is a maximal compact subgroup of G′. An important problem in branching theory is to classify∩ the reductive Lie group pairs (G, G′) such that there exists at least one nontrivial unitarizable simple (g,K)-module that is discretely decomposable as a (g′,K′)-module. If G′ is compact, this always holds obviously. Hence in this article, the author will only considers the cases when G′ is noncompact. If (G, G′) is a symmetric pair, the problem was solved completely by Toshiyuki KOBAYASHI and Yoshiki OSHIMA¯ in [11, Corollary 5.8].