Lie Theory and the Chern–Weil Homomorphism
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Nilpotent Lie Groups and Hyperbolic Automorphisms ”
Nilpotent Lie groups and hyperbolic automorphisms Manoj Choudhuri and C. R. E. Raja Abstract A connected Lie group admitting an expansive automorphism is known to be nilotent, but all nilpotent Lie groups do not admit expansive au- tomorphism. In this article, we find sufficient conditions for a class of nilpotent Lie groups to admit expansive automorphism. Let G be a locally compact (second countable) group and Aut(G) be the group of (continuous) automorphisms of G. We consider automorphisms α of G that have a specific property that there is a neighborhood U of identity such that n ∩n∈Zα (U) = {e} - such automorphisms are known as expansive. The struc- ture of compact connected groups admitting expansive automorphism has been studied in [6], [7], [17], [10] and it was shown in [10] that a compact connected group admitting an expansive automorphism is abelian. The same problen has been studied for totally disconnected groups as well, see [9] and [16] for com- pact totally disconnected groups and a recent paper of Helge Glockner and the second named author ([8]) for locally compact totally disconnected groups. In [14], Riddhi Shah has shown that a connected locally compact group admitting expansive automorphism is nilpotent. The result was known previously for Lie groups (see Proposition 7.1 of [8] or Proposition 2.2 of [14] for a proof of this fact and further references). But all nilpotent Lie groups do not admit expansive automorphism which can be seen easily by considering the circle group. In this article, we try to classify a class of nilpotent Lie groups which admit expansive automorphism. -
Homological Stability of Diffeomorphism Groups 3
HOMOLOGICAL STABILITY OF DIFFEOMORPHISM GROUPS ALEXANDER BERGLUND AND IB MADSEN Abstract. In this paper we prove a stability theorem for block diffeomor- phisms of 2d-dimensional manifolds that are connected sums of Sd ×Sd. Com- bining this with a recent theorem of S. Galatius and O. Randal-Williams and Morlet’s lemma of disjunction, we determine the homology of the classifying space of their diffeomorphism groups relative to an embedded disk in a stable range. Dedicated to Dennis Sullivan on the occasion of his 70th birthday 1. Introduction The traditional method to obtain homotopical and homological information about diffeomorphism groups of high dimensional smooth manifolds is a two step procedure: the surgery exact sequence handles the larger group of block diffeomor- phisms and Waldhausen’s K-theory of spaces connects block diffeomorphisms and actual diffeomorphisms. In practice one is forced to retreat to rational information. The method was used by Farrell and Hsiang [17] to evaluate the rational homotopy groups of the orientation preserving diffeomorphism groups of spheres in a modest range of dimensions; Q, k ≡ 0 (4), n even n (1) πk(B Diff(S )) ⊗ Q = Q ⊕ Q, k ≡ 0 (4), n odd 0, otherwise. n n for 0 <k< 6 − 7. The orthogonal group SO(n + 1) is a subgroup of Diff(S ), and πkSO(n + 1) accounts for one Q when k ≡ 0 (4). The second Q in line two above is of a different nature. It comes from the connection between Waldhausen’s algebraic K-theory of spaces and the homotopy theory of the homogeneous space Diff(Sn)/ Diff(Sn) of block diffeomorphisms modulo diffeomorphisms. -
Clifford Algebras and the Classical Dynamical Yang-Baxter Equation
Mathematical Research Letters 10, 253–268 (2003) CLIFFORD ALGEBRAS AND THE CLASSICAL DYNAMICAL YANG-BAXTER EQUATION A. Alekseev and E. Meinrenken Abstract. We describe a relationship of the classical dynamical Yang-Baxter equation with the following elementary problem for Clifford algebras: Given a vector space V with quadratic form QV , how is the exponential of an element in ∧2(V ) under exterior algebra multiplication related to its exponential under Clifford multiplication? 1. Introduction Let g be a real Lie algebra, equipped with a non-degenerate invariant qua- dratic form Q. Let Θ ∈∧3g be the cubic element defined by the quadratic form and the Lie algebra structure. An element r ∈∧2g is called a classical r-matrix for g if it satisfies the (modified) classical Yang-Baxter equation (CYBE) 1 [r, r]g = Θ 2 for some coupling constant ∈ R. Here [r, r]g is defined using the extension of the Lie bracket to the Schouten bracket on the exterior algebra, [·, ·]g : ∧kg × ∧lg →∧k+l−1g. Drinfeld [8] and Semenov-Tian-Shansky [20] gave a geometric interpretation of the CYBE in terms of Poisson-Lie group structures, and a classification of r-matrices for semi-simple Lie algebras and = 0 was obtained by Belavin-Drinfeld [6]. The CYBE admits an important generalization known as the classical dynam- ical Yang-Baxter equation (CDYBE). Let k ⊂ g be a Lie subalgebra. A classical dynamical r-matrix is a k-equivariant (meromorphic)function r : k∗ →∧2g satisfying the (modified)CDYBE [11] ∂r 1 ∧ e + [r, r]g = Θ. ∂µ i 2 i i i ∗ Here ei is a basis on k with dual basis e ∈ k , and µi are the corresponding coordinates on k∗. -
A Mathematical Approach to Wick Rotations
A mathematical approach to Wick rotations by Christer Helleland Thesis submitted in fulfilment of the requirements for the degree of PHILOSOPHIAE DOCTOR (PhD) ! Faculty of Science and Technology Department of Mathematics and Physics 2019 University of Stavanger NO-4036 Stavanger NORWAY www.uis.no ©2019 Christer Helleland ISBN: Click to enter ISBN. ISSN: Click to enter ISSN. PhD: Thesis UiS No. Click to enter PhD No. Contents List of Tables6 Acknowledgements8 Part 1. Introduction 9 Part 2. Preliminaries 12 1. Cartan involutions of linear Lie groups 12 2. Geometric invariant theory (GIT) 16 Part 3. Wick-rotations and real GIT 22 1. Introduction 22 2. Mathematical Preliminaries 23 2.1. Real form of a complex vector space 23 2.2. Real slices 24 2.3. Compatible real forms 25 3. Holomorphic Riemannian manifolds 27 3.1. Complexification of real manifolds 27 3.2. Complex differential geometry 28 3.3. Real slices from a frame-bundle perspective 29 4. Lie groups 31 4.1. Complex Lie groups and their real forms 31 4.2. Example: Split G2-holonomy manifolds 32 5. A standard Wick-rotation to a real Riemannian space 34 5.1. Minimal vectors and closure of real semi-simple orbits 34 5.2. Compatible triples and intersection of real orbits 36 5.3. The real Riemannian case 37 5.4. The adjoint action of the Lorentz groups O(n − 1; 1) 38 5.5. Uniqueness of real orbits and the class of complex Lie groups 41 6. Applications to the pseudo-Riemannian setting 45 6.1. Pseudo-Riemannian examples 47 Acknowledgements 48 Appendix A. -
On 2-Plectic Lie Groups
On 2-plectic Lie groups Mohammad Shafiee and Masoud Aminizadeh Abstract. A 2-plectic Lie group is a Lie group endowed with a 2-plectic structure which is left invariant. In this paper we provide some inter- esting examples of 2-plectic Lie groups. Also we study the structure of the set of Hamiltonian covectors and vectors of a 2-plectic Lie algebra. Moreover, the existence of i-isotropic and i-Lagrangian subgroups are in- vestigated. At last we obtain some results about the reduction of some 2-plectic structures. M.S.C. 2010: 53D05, 17B60. Key words: 2-plectic structure; quadratic Lie algebra; Hamiltonian vector. 1 Introduction A k-plectic manifold (M; !) is a smooth manifold M endowed with a (k + 1)-form ! which is closed and nondegenerate in the sense that ιX ! = 0, X 2 TM, implies that X = 0. In this case ! is called a k-plectic structure. These structures are general version of symplectic structures and they naturally appear in the Hamiltonian formulation of classical fields (see [4]and references therein ). Mathematically, in spite of general case, symplectic structures are very interesting and so they have been studied extensively. However, in recent years, 2-plectic structures also have been considered and these structures also are studied extensively ([1], [8]). An important class of 2-plectic manifolds are 2-plectic Lie groups. Similar to symplectic case, a 2-plectic Lie group is defined as follows. Definition 1.1. A 2-plectic Lie group (G; !) is a Lie group G endowed with a 2- plectic structure ! which is left invariant. -
Clifford Algebras and Lie Groups Lecture Notes, University of Toronto
Clifford algebras and Lie groups Eckhard Meinrenken Lecture Notes, University of Toronto, Fall 2009. Last revision: 12/2011 Contents Chapter 1. Symmetric bilinear forms 7 1. Quadratic vector spaces 7 2. Isotropic subspaces 9 3. Split bilinear forms 10 4. E.Cartan-Dieudonn´e'sTheorem 13 5. Witt's Theorem 16 6. Orthogonal groups for K = R; C 17 7. Lagrangian Grassmannians 23 Chapter 2. Clifford algebras 27 1. Exterior algebras 27 1.1. Definition 27 1.2. Universal property, functoriality 28 2. Clifford algebras 29 2.1. Definition and first properties 30 2.2. Universal property, functoriality 31 2.3. The Clifford algebras Cl(n; m) 32 2.4. The Clifford algebras Cl(n) 33 2.5. Symbol map and quantization map 34 2.6. Transposition 35 2.7. Chirality element 36 2.8. The trace and the super-trace 37 2.9. Extension of the bilinear form 38 2.10. Lie derivatives and contractions 38 2.11. The Lie algebra q(^2(V )) 40 2.12. A formula for the Clifford product 41 3. The Clifford algebra as a quantization of the exterior algebra 42 3.1. Differential operators 42 3.2. Graded Poisson algebras 44 3.3. Graded super Poisson algebras 45 3.4. Poisson structures on ^(V ) 46 Chapter 3. The spin representation 49 1. The Clifford group and the spin group 49 1.1. The Clifford group 49 1.2. The groups Pin(V ) and Spin(V ) 51 2. Clifford modules 54 2.1. Basic constructions 54 2.2. The spinor module SF 56 2.3. -
Semibounded Unitary Representations of Double Extensions of Hilbert–Loop Groups Tome 64, No 5 (2014), P
R AN IE N R A U L E O S F D T E U L T I ’ I T N S ANNALES DE L’INSTITUT FOURIER K. H. NEEB Semibounded Unitary Representations of Double Extensions of Hilbert–Loop Groups Tome 64, no 5 (2014), p. 1823-1892. <http://aif.cedram.org/item?id=AIF_2014__64_5_1823_0> © Association des Annales de l’institut Fourier, 2014, tous droits réservés. L’accès aux articles de la revue « Annales de l’institut Fourier » (http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/). Toute re- production en tout ou partie de cet article sous quelque forme que ce soit pour tout usage autre que l’utilisation à fin strictement per- sonnelle du copiste est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ Ann. Inst. Fourier, Grenoble 64, 5 (2014) 1823-1892 SEMIBOUNDED UNITARY REPRESENTATIONS OF DOUBLE EXTENSIONS OF HILBERT–LOOP GROUPS by K. H. NEEB (*) Abstract. — A unitary representation π of a, possibly infinite dimensional, Lie group G is called semibounded if the corresponding operators idπ(x) from the derived representation are uniformly bounded from above on some non-empty open subset of the Lie algebra g of G. We classify all irreducible semibounded represen- tations of the groups Lbφ(K) which are double extensions of the twisted loop group Lφ(K), where K is a simple Hilbert–Lie group (in the sense that the scalar product on its Lie algebra is invariant) and φ is a finite order automorphism of K which leads to one of the 7 irreducible locally affine root systems with their canonical Z-grading. -
Dirac Operators in Representation Theory
Jing-Song Huang and Pavle Pandˇzi´c Dirac Operators in Representation Theory SPIN Springer’s internal project number, if known – Monograph – December 14, 2005 Springer Berlin Heidelberg NewYork Hong Kong London Milan Paris Tokyo Preface We begin with the origin of the Dirac equation and give a brief introduction of the Dirac operators due to Parthasarathy, Vogan and Kostant. Then we explain a conjecture of Vogan on Dirac cohomology, which we proved in [HP1], its applications and the organization of the book. 0.1 The Dirac equation. The Dirac equation has an interesting connection to E = mc2, the Einstein’s equation from his special theory of relativity. This equation relates the energy E of a particle at rest to its mass m through a conversion factor, the square of the speed c of light. However, this way of writing the equation obscures the underlying four-dimensional geometry. The relation for a particle in motion is a hyperbolic equation: E2 c2p p = (mc2)2. (0.1) − · Here the energy E is the first component of a vector (E,cp) = (E,cp1,cp2,cp3) and p is the vector that describes the momentum of the particle. This more general equation exhibits the mechanism of the conversion of mass into relative motion. 1 For describing relativistic spin 2 particles Dirac was to rewrite the quadratic Einstein relation (0.1) as a linear relation. This would seem impossible. But Dirac came up with a new idea by writing the relation as follows: 3 2 γ0E + c γj pj = mc I, (0.2) j=1 X where γ (k =0, 1, 2, 3) are 4 4 matrices and I is the 4 4 identity matrix. -
The Fourier Transform for Nilpotent Locally Compact Groups. I
Pacific Journal of Mathematics THE FOURIER TRANSFORM FOR NILPOTENT LOCALLY COMPACT GROUPS. I ROGER EVANS HOWE Vol. 73, No. 2 April 1977 PACIFIC JOURNAL OF MATHEMATICS Vol. 73, No. 2, 1977 THE FOURIER TRANSFORM FOR NILPOTENT LOCALLY COMPACT GROUPS: I ROGER E. HOWE In his work on nilpotent lie groups, A. A. Kirillov intro- duced the idea of classifying the representations of such groups by matching them with orbits in the dual of the lie algebra under the coadjoint action. His methods have proved extremely fruitful, and subsequent authors have refined and extended them to the point where they provide highly satisfac- tory explanations of many aspects of the harmonic analysis of various lie groups. Meanwhile, it appears that nonlie groups are also amenable to such an approach. In this paper, we seek to indicate that, indeed, a very large class of separable, locally compact, nilpotent groups have a Kirillov- type theory. On the other hand, elementary examples show that not all such groups can have a perfect Kirillov theory. The precise boundary between good and bad groups is not well defined, and varies with the amount of technical complication you can tolerate. At this stage, the delineation of the boundary is the less rewarding part of the theory, and will be deferred to a future publication. In the present paper, we lay some groundwork, and then discuss a particularly nice special case, which also has significance in the general picture. Since Kirillov's approach hinges on the use of the lie algebra and its dual, the first concern in imitating his theory is to find a lie algebra. -
An Introduction to Lie Algebras and the Theorem of Ado
An introduction to Lie algebras and the theorem of Ado Hofer Joachim 28.01.2012 An introduction to Lie algebras and the theorem of Ado Contents Introduction 2 1 Lie algebras 3 1.1 Subalgebras, ideals, quotients . 4 1.2 Nilpotent, solvable, simple and semisimple Lie algebras . 5 2 The representation theory of Lie algebras 7 2.1 Examples . 7 2.2 Modules, submodules, quotient modules . 7 2.3 Structure theorems: Lie and Engel . 8 3 The theorem of Ado for nilpotent Lie algebras. How can a faithful representation be constructed? 11 3.1 Ad hoc examples . 11 3.2 The universal enveloping algebra . 11 3.2.1 Tensor products and the tensor algebra . 11 3.2.2 The universal enveloping algebra of a Lie algebra . 12 3.2.3 The Poincare-Birkhoff-Witt theorem . 12 3.3 Constructing a faithful representation of h1 ............................... 12 3.4 Ado’s theorem for nilpotent Lie algebras . 13 3.5 Constructing a faithful representation for the standard filiform Lie algebra of dimension 4 . 14 3.6 Constructing a faithful representation for an abelian Lie algebra . 15 4 The theorem of Ado 16 4.1 Derivations . 16 4.2 Direct and semidirect sums of Lie algebras . 16 4.3 Proof of Ado’s theorem . 17 4.4 Proof of Neretin’s lemma . 18 4.5 Constructing a faithful representation of the 2-dimensional upper triangular matrices . 19 4.6 Constructing a faithful representation of an abstract Lie algebra . 19 1 Hofer Joachim An introduction to Lie algebras and the theorem of Ado Introduction Lie groups and Lie algebras are of great importance in modern physics, particularly in the context of (continu- ous) symmetry transformations. -
Representation Theory in Complex Rank, II
Representation theory in complex rank, II The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation Etingof, Pavel. “Representation Theory in Complex Rank, II.” Advances in Mathematics 300 (September 2016): 473–504 © 2016 Elsevier Inc As Published http://dx.doi.org/10.1016/J.AIM.2016.03.025 Publisher Elsevier BV Version Author's final manuscript Citable link http://hdl.handle.net/1721.1/118626 Terms of Use Creative Commons Attribution-NonCommercial-NoDerivs License Detailed Terms http://creativecommons.org/licenses/by-nc-nd/4.0/ REPRESENTATION THEORY IN COMPLEX RANK, II PAVEL ETINGOF To the memory of Andrei Zelevinsky 1. Introduction Let Ct be one of the categories Rep(St), Rep(GLt), Rep(Ot), Rep(Sp2t), obtained by interpolating the classical representation categories Rep(Sn), Rep(GLn), Rep(On), Rep(Sp2n) to complex values of n, defined by Deligne-Milne and Deligne ([DM, De1, De2]).1 In [E1], by analogy with the representation theory of real reductive groups, we proposed to consider various categories of “Harish-Chandra modules” based on Ct, whose objects M are objects of Ct equipped with additional mor- phisms satisfying certain relations. In this situation, the structure of an object of Ct on M is analogous to the action of the “maximal com- pact subgroup”, while the additional morphisms play the role of the “noncompact part”. The papers [E1, EA, Ma] study examples of such categories based on the category Rep(St) (which could be viewed as do- ing “algebraic combinatorics in complex rank”). This paper is a sequel to these works, and its goal is to start developing “Lie theory in complex rank”, extending the constructions of [E1] to “Lie-theoretic” categories Rep(GLt), Rep(Ot), Rep(Sp2t) (based on the ideas outlined in [E2]). -
Lie Algebras with Ad-Invariant Metrics. a Survey
LIE ALGEBRAS WITH AD-INVARIANT METRICS A SURVEY GABRIELA P. OVANDO Abstract. This is a survey work on Lie algebras with ad-invariant met- rics. We summarize main features, notions and constructions, in the aim of bringing into consideration the main research on the topic. We also give some list of examples in low dimensions. To the memory of our friend Sergio 1. Introduction An ad-invariant metric on a Lie algebra g is a non-degenerate symmetric bilinear form h , i which satisfies (1) h[x, y], zi + hy, [x, z]i = 0 for all x, y, z ∈ g. Lie algebras equipped with ad-invariant metrics are known as: “metric”[22], “metrised” [10], “orthogonal” [28], “quadratic” [27], “regular quadratic”[16], ”symmetric self-dual” [17], ”self-dual” [36] Lie algebras. Lie algebras which can be endowed with an ad-invariant metric are also known as “quadrable” or “metrisable”. They became relevant some years ago when they were useful in the formulation of some physical problems, for instance in the so known Adler-Kostant-Symes scheme. More recently they appeared in conformal field theory precisely as the Lie algebras for which a Sugawara construction exists [17]. They also constitute the basis for the construction of bi-algebras and they arXiv:1512.03997v2 [math.DG] 14 Jun 2017 give rise to interesting pseudo-Riemannian geometry [13]. For instance in [34] a result originally due to Kostant [26] was revalidated for pseudo-Riemannian metrics: it states that there exists a Lie group acting by isometries on a pseudo- Riemannian naturally reductive space (in particular symmetric spaces) whose Lie algebra can be endowed with an ad-invariant metric.