Symmetric Spaces of Hermitian Type
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The Pure State Space of Quantum Mechanics As Hermitian Symmetric
The Pure State Space of Quantum Mechanics as Hermitian Symmetric Space. R. Cirelli, M. Gatti, A. Mani`a Dipartimento di Fisica, Universit`adegli Studi di Milano, Italy Istituto Nazionale di Fisica Nucleare, Sezione di Milano, Italy Abstract The pure state space of Quantum Mechanics is investigated as Hermitian Symmetric K¨ahler manifold. The classical principles of Quantum Mechan- ics (Quantum Superposition Principle, Heisenberg Uncertainty Principle, Quantum Probability Principle) and Spectral Theory of observables are dis- cussed in this non linear geometrical context. Subj. Class.: Quantum mechanics 1991 MSC : 58BXX; 58B20; 58FXX; 58HXX; 53C22 Keywords: Superposition principle, quantum states; Riemannian mani- folds; Poisson algebras; Geodesics. 1. Introduction Several models of delinearization of Quantum Mechanics have been pro- arXiv:quant-ph/0202076v1 14 Feb 2002 posed (see f.i. [20] [26], [11], [2] and [5] for a complete list of references). Frequentely these proposals are supported by different motivations, but it appears that a common feature is that, more or less, the delinearization must be paid essentially by the superposition principle. This attitude can be understood if the delinearization program is worked out in the setting of a Hilbert space as a ground mathematical structure. However, as is well known, the groundH mathematical structure of QM is the manifold of (pure) states P( ), the projective space of the Hilbert space . Since, obviously, P( ) is notH a linear object, the popular way of thinking thatH the superposition principleH compels the linearity of the space of states is untenable. The delinearization program, by itself, is not related in our opinion to attempts to construct a non linear extension of QM with operators which 1 2 act non linearly on the Hilbert space . -
Symmetric Spaces with Conformal Symmetry
Symmetric Spaces with Conformal Symmetry A. Wehner∗ Department of Physics, Utah State University, Logan, Utah 84322 October 30, 2018 Abstract We consider an involutive automorphism of the conformal algebra and the resulting symmetric space. We display a new action of the conformal group which gives rise to this space. The space has an in- trinsic symplectic structure, a group-invariant metric and connection, and serves as the model space for a new conformal gauge theory. ∗Electronic-mail: [email protected] arXiv:hep-th/0107008v1 1 Jul 2001 1 1 Introduction Symmetric spaces are the most widely studied class of homogeneous spaces. They form a subclass of the reductive homogeneous spaces, which can es- sentially be characterized by the fact that they admit a unique torsion-free group-invariant connection. For symmetric spaces the curvature is covari- antly constant with respect to this connection. Many essential results and extensive bibliographies on symmetric spaces can be found, for example, in the standard texts by Kobayashi and Nomizu [1] and Helgason [2]. The physicists’ definition of a (maximally) symmetric space as a metric space which admits a maximum number of Killing vectors is considerably more restrictive. A thorough treatment of symmetric spaces in general rel- ativity, where a pseudo-Riemannian metric and the metric-compatible con- nection are assumed, can be found in Weinberg [3]. The most important symmetric space in gravitational theories is Minkowski space, which is based on the symmetric pair (Poincar´egroup, Lorentz group). Since the Poincar´e group is not semi-simple, it does not admit an intrinsic group-invariant met- ric, which would project in the canonical fashion to the Minkowski metric ηab = diag(−1, 1 .. -
LIE GROUPS and ALGEBRAS NOTES Contents 1. Definitions 2
LIE GROUPS AND ALGEBRAS NOTES STANISLAV ATANASOV Contents 1. Definitions 2 1.1. Root systems, Weyl groups and Weyl chambers3 1.2. Cartan matrices and Dynkin diagrams4 1.3. Weights 5 1.4. Lie group and Lie algebra correspondence5 2. Basic results about Lie algebras7 2.1. General 7 2.2. Root system 7 2.3. Classification of semisimple Lie algebras8 3. Highest weight modules9 3.1. Universal enveloping algebra9 3.2. Weights and maximal vectors9 4. Compact Lie groups 10 4.1. Peter-Weyl theorem 10 4.2. Maximal tori 11 4.3. Symmetric spaces 11 4.4. Compact Lie algebras 12 4.5. Weyl's theorem 12 5. Semisimple Lie groups 13 5.1. Semisimple Lie algebras 13 5.2. Parabolic subalgebras. 14 5.3. Semisimple Lie groups 14 6. Reductive Lie groups 16 6.1. Reductive Lie algebras 16 6.2. Definition of reductive Lie group 16 6.3. Decompositions 18 6.4. The structure of M = ZK (a0) 18 6.5. Parabolic Subgroups 19 7. Functional analysis on Lie groups 21 7.1. Decomposition of the Haar measure 21 7.2. Reductive groups and parabolic subgroups 21 7.3. Weyl integration formula 22 8. Linear algebraic groups and their representation theory 23 8.1. Linear algebraic groups 23 8.2. Reductive and semisimple groups 24 8.3. Parabolic and Borel subgroups 25 8.4. Decompositions 27 Date: October, 2018. These notes compile results from multiple sources, mostly [1,2]. All mistakes are mine. 1 2 STANISLAV ATANASOV 1. Definitions Let g be a Lie algebra over algebraically closed field F of characteristic 0. -
Holonomy and the Lie Algebra of Infinitesimal Motions of a Riemannian Manifold
HOLONOMY AND THE LIE ALGEBRA OF INFINITESIMAL MOTIONS OF A RIEMANNIAN MANIFOLD BY BERTRAM KOSTANT Introduction. .1. Let M be a differentiable manifold of class Cx. All tensor fields discussed below are assumed to be of class C°°. Let X be a vector field on M. If X vanishes at a point oCM then X induces, in a natural way, an endomorphism ax of the tangent space F0 at o. In fact if y£ V„ and F is any vector field whose value at o is y, then define axy = [X, Y]„. It is not hard to see that [X, Y]0 does not depend on F so long as the value of F at o is y. Now assume M has an affine connection or as we shall do in this paper, assume M is Riemannian and that it possesses the corresponding affine connection. One may now associate to X an endomorphism ax of F0 for any point oCM which agrees with the above definition and which heuristically indicates how X "winds around o" by defining for vC V0, axv = — VtX, where V. is the symbol of covariant differentiation with respect to v. X is called an infinitesmal motion if the Lie derivative of the metric tensor with respect to X is equal to zero. This is equivalent to the statement that ax is skew-symmetric (as an endomorphism of F0 where the latter is provided with the inner product generated by the metric tensor) for all oCM. §1 contains definitions and formulae which will be used in the remaining sections. -
Symmetric Spaces
CHAPTER 2 Symmetric Spaces Introduction We remark that a prerequisite for this course is a basic understanding of Rie- mannian geometry, see for instance [Boo86]or[Hel79], which at the same time is a standard reference for the theory of symmetric spaces. See also [Bor98]fora much more condensed version of the latter. In 1926, É. Cartan began to study those Riemannian manifolds,forwhich central symmetries are distance preserving. The term central symmetry is going to be made precise later but you can think of it as a reflection about a point, as in Rn for instance. These spaces are now known as symmetric spaces;henoticedthatthe classification of these is essentially equivalent to the classification of real semisimple Lie algebras. The local definition of symmetric spaces is a generalisation of constant sectional curvature. Just as a differentiable function from R to R is constant if its derivative vanishes identically, one may ask for the Riemanncurvaturetensorto have covariant derivative zero. As incomprehensible as thisstatementmaybeatthe moment, it yields an important equivalent characterizationofsymmetricspaces. Example. The following list of examples of symmetric spaces contains the constant curvature cases. n n (i) Euclidean n-space E =(R ,geucl) has constant sectional curvature zero and isometry group Iso(En) = O(n) !Rn. n n ∼ (ii) The n-sphere S =(S ,geucl) has constant sectional curvature one. Its Riemannian metric arises through restriction of the Riemannian metric of the ambient space Rn+1 Sn to the tangent bundle of Sn.Theisometry group of Sn is O(n). ⊃ (iii) Hyperbolic n-space Hn has constant sectional curvature minus one. -
Linear Algebraic Groups
Clay Mathematics Proceedings Volume 4, 2005 Linear Algebraic Groups Fiona Murnaghan Abstract. We give a summary, without proofs, of basic properties of linear algebraic groups, with particular emphasis on reductive algebraic groups. 1. Algebraic groups Let K be an algebraically closed field. An algebraic K-group G is an algebraic variety over K, and a group, such that the maps µ : G × G → G, µ(x, y) = xy, and ι : G → G, ι(x)= x−1, are morphisms of algebraic varieties. For convenience, in these notes, we will fix K and refer to an algebraic K-group as an algebraic group. If the variety G is affine, that is, G is an algebraic set (a Zariski-closed set) in Kn for some natural number n, we say that G is a linear algebraic group. If G and G′ are algebraic groups, a map ϕ : G → G′ is a homomorphism of algebraic groups if ϕ is a morphism of varieties and a group homomorphism. Similarly, ϕ is an isomorphism of algebraic groups if ϕ is an isomorphism of varieties and a group isomorphism. A closed subgroup of an algebraic group is an algebraic group. If H is a closed subgroup of a linear algebraic group G, then G/H can be made into a quasi- projective variety (a variety which is a locally closed subset of some projective space). If H is normal in G, then G/H (with the usual group structure) is a linear algebraic group. Let ϕ : G → G′ be a homomorphism of algebraic groups. Then the kernel of ϕ is a closed subgroup of G and the image of ϕ is a closed subgroup of G. -
Strongly Exponential Symmetric Spaces
STRONGLY EXPONENTIAL SYMMETRIC SPACES YANNICK VOGLAIRE Abstract. We study the exponential map of connected symmetric spaces and characterize, in terms of midpoints and of infinitesimal conditions, when it is a diffeomorphism, generalizing the Dixmier–Saito theorem for solvable Lie groups. We then give a geometric characterization of the (strongly) exponential solvable symmetric spaces as those spaces for which every triangle admits a unique double triangle. This work is motivated by Weinstein’s quantization by groupoids program applied to symmetric spaces. 1. Introduction In the late 1950’s, Dixmier [5] and Saito [16] characterized the strongly exponential Lie groups: the simply connected solvable Lie groups for which the exponential map is a global diffeomorphism. They are characterized by the fact that the exponential map is either injective or surjective, or equivalently the fact that the adjoint action of their Lie algebra has no purely imaginary eigenvalue. In contrast, the exponential map of semisimple Lie groups is never injective, but may be surjective or have dense image. As a result, the latter two weaker notions of exponentiality have been studied for general Lie groups by a number of authors (see [6, 21] for two surveys and for references). Recently, a number of their results were generalized to symmetric spaces in [15]. The first main result of the present paper intends to complete the picture by giving a version of the Dixmier–Saito theorem for symmetric spaces (see Theorems 1.1, 1.2 and 1.3). The second main result gives a geometric characterization of the strongly ex- arXiv:1303.5925v2 [math.DG] 6 Apr 2014 ponential symmetric spaces which are homogeneous spaces of solvable Lie groups, in terms of existence and uniqueness of double triangles (see Theorem 1.4). -
Symmetric Submanifolds of Symmetric Spaces 11
SYMMETRIC SUBMANIFOLDS OF SYMMETRIC SPACES JURGENÄ BERNDT Abstract. This paper contains a survey about the classi¯cation of symmetric subman- ifolds of symmetric spaces. It is an extended version of a talk given by the author at the 7th International Workshop on Di®erential Geometry at Kyungpook National University in Taegu, Korea, in November 2002. 1. Introduction A connected Riemannian manifold M is a symmetric space if for each point p 2 M there exists an involutive isometry sp of M such that p is an isolated ¯xed point of M. Symmetric spaces play an important role in Riemannian geometry because of their relations to algebra, analysis, topology and number theory. The symmetric spaces have been classi¯ed by E. Cartan. A thorough introduction to symmetric spaces can be found in [4]. Symmetric submanifolds play an analogous role in submanifold geometry. The precise de¯nition of a symmetric submanifold is as follows. A submanifold S of a Riemannian manifold M is a symmetric submanifold of M if for each point p 2 S there exists an involutive isometry σp of M such that ( ¡X , if X 2 TpS; σp(p) = p ; σp(S) = S and (σp)¤(X) = X , if X 2 ºpS: Here, TpS denotes the tangent space of S at p and ºpS the normal space of S at p. The isometry σp is called the extrinsic symmetry of S at p. It follows from the very de¯nition that a symmetric submanifold is a symmetric space. The aim of this paper is to present a survey about the classi¯cation problem of symmetric submanifolds of symmetric spaces. -
Complex-Symmetric Spaces Annales De L’Institut Fourier, Tome 39, No 2 (1989), P
ANNALES DE L’INSTITUT FOURIER RALF LEHMANN Complex-symmetric spaces Annales de l’institut Fourier, tome 39, no 2 (1989), p. 373-416 <http://www.numdam.org/item?id=AIF_1989__39_2_373_0> © Annales de l’institut Fourier, 1989, tous droits réservés. L’accès aux archives de la revue « Annales de l’institut Fourier » (http://annalif.ujf-grenoble.fr/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une in- fraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. Inst. Fourier, Grenoble 39, 2 (1989), 373-416. COMPLEX-SYMMETRIC SPACES by Ralf LEHMANN 0. Introduction. Let M be a complete complex Hermitian manifold. Then M is called a Hermitian symmetric space, if and only if for every x e M there exists a holomorphic isometry of order two which has x as an isolated fixed point. This condition immediately implies that the group of holomorphic isometries acts transitively on M and that the Hermitian metric is Kahlerian. Moreover, each compact Hermitian symmetric space can be written as a product of a compact torus and a homogeneous projective rational manifold which is Hermitian symmetric. These manifolds are classified by using the classification of semisimple Lie algebras (see e.g. [Hel] and [Ca]). Generalizations of symmetric spaces to the infinite-dimensional case have turned out to be very interesting (see e.g. [K]). We are concerned here with manifolds where the isometry condition is dropped. -
Nilpotent Orbits and Theta-Stable Parabolic Subalgebras
REPRESENTATION THEORY An Electronic Journal of the American Mathematical Society Volume 2, Pages 1{32 (February 3, 1998) S 1088-4165(98)00038-7 NILPOTENT ORBITS AND THETA-STABLE PARABOLIC SUBALGEBRAS ALFRED G. NOEL¨ Abstract. In this work, we present a new classification of nilpotent orbits in a real reductive Lie algebra g under the action of its adjoint group. Our classification generalizes the Bala-Carter classification of the nilpotent orbits of complex semisimple Lie algebras. Our theory takes full advantage of the work of Kostant and Rallis on p , the “complex symmetric space associated C with g”. The Kostant-Sekiguchi correspondence, a bijection between nilpotent orbits in g and nilpotent orbits in p , is also used. We identify a fundamental C set of noticed nilpotents in p and show that they allow us to recover all other C nilpotents. Finally, we study the behaviour of a principal orbit, that is an orbit of maximal dimension, under our classification. This is not done in the other classification schemes currently available in the literature. Introduction Let g be a semisimple Lie algebra and G its adjoint group. We say that an C C element x of g is nilpotent if and only if, ad : y [x; y] for all y g ,isa C x C nilpotent endomorphism of g . Kostant (see also Dynkin→ [Dy]) has shown,∈ in his C fundamental 1959 paper [Ko], that the number of nilpotent orbits of G in g is C C finite. The Bala-Carter classification can be expressed as follows: There is a one-to-one correspondence between nilpotent orbits of g and con- C jugacy classes of pairs (m; p ), where m is a Levi subalgebra of g and p is a m C m distinguished parabolic subalgebra of the semisimple algebra [m; m]. -
The Symmetric Space for Sln(R)
The Symmetric Space for SLn(R) Rich Schwartz November 27, 2013 The purpose of these notes is to discuss the symmetric space X on which SLn(R) acts. Here, as usual, SLn(R) denotes the group of n × n matrices of determinant 1. 1 The Group Action The space X denotes the sets of n × n real matrices M such that • M is symmetric: M t = M. • det(M)=1. • M is positive definite: M(v) · v > 0 for all v =6 0. The action of SLn(R) on X is given by g(M)= gMgt. (1) One can easily verify that g(M) ∈ X. Only the third step has anything to it: gMgt(v) · v = M(gt(v)) · gt(v)= M(w) · w> 0. The action we have described really is a group action, because g(h(M)) = g(hMht)gt =(gh)M(gh)t = gh(M). 1 2 The Tangent Space The identity matrix I is the natural origin for X. The tangent space TI (X) consists of derivatives of the form dM V = (0), (2) ds where Ms is a path of matrices in X and M0 = I. Clearly V is a symmetric matrix. Also, to first order, we have Ms = I + sV , and det(I + sV )=1+ s trace(V )+ ... (3) Hence trace(V ) = 0. Conversely, if trace(V ) = 0 and V is symmetric, then I + sV belongs to X to first order. More precisely s2 s3 M = exp(sV )= I + sV + V 2 + V 3 + ··· (4) s 2! 3! gives a path in X, for small s, having V as derivative. -
Finiteness of Orbit Structure for Real Flag Manifolds
JOSEPH A. WOLF* FINITENESS OF ORBIT STRUCTURE FOR REAL FLAG MANIFOLDS ABSTRACT. Let G be a reductive real Lie group, a an involutive automorphism of (7, and L = G u the fixed point set of a. It is shown that G has only finitely many L-conjugacy classes of parabolic subgroups, so if P is a parabolic subgroup of G then there are only finitely many L-orbits on the real flag manifold G/P. This is done by showing that G has only finitely many L-conjugacy classes of a-stable Cartan subgroups. These results extend known facts for the case where G is a complex group and L is a real form of G. Key words and phrases: flag manifold, reductive Lie group, semisimple Lie group, para- bolic subgroup, Caftan subgroup, Cartan subalgebra. AMS Subject Classification (1970) Primary: 22-50, 22-70, 53-66 Secondary: 14-45, 57-47 1. INTRODUCTION One knows [4] that there are only finitely many conjugacy classes of Cartan subalgebras in a reductive real Lie algebra. If G is a complex reductive Lie group and L is a real form, it follows [8] that there are only finitely many L-eonjugacy classes of parabolic subgroups of G. In particular, if X= G/P is a complex flag manifold of G, then [8] there are only finitely many L-orbits on X. Here we extend these results to the case where G is a reductive real Lie group and L is the fixed point set of an involutive automorphism, and we indicate the scope of applicability of the extension.