Symmetric, Invariant, Non-Degenerate Bilinear Form on a Lie Algebra
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Topological Vector Spaces and Algebras
Joseph Muscat 2015 1 Topological Vector Spaces and Algebras [email protected] 1 June 2016 1 Topological Vector Spaces over R or C Recall that a topological vector space is a vector space with a T0 topology such that addition and the field action are continuous. When the field is F := R or C, the field action is called scalar multiplication. Examples: A N • R , such as sequences R , with pointwise convergence. p • Sequence spaces ℓ (real or complex) with topology generated by Br = (a ): p a p < r , where p> 0. { n n | n| } p p p p • LebesgueP spaces L (A) with Br = f : A F, measurable, f < r (p> 0). { → | | } R p • Products and quotients by closed subspaces are again topological vector spaces. If π : Y X are linear maps, then the vector space Y with the ini- i → i tial topology is a topological vector space, which is T0 when the πi are collectively 1-1. The set of (continuous linear) morphisms is denoted by B(X, Y ). The mor- phisms B(X, F) are called ‘functionals’. +, , Finitely- Locally Bounded First ∗ → Generated Separable countable Top. Vec. Spaces ///// Lp 0 <p< 1 ℓp[0, 1] (ℓp)N (ℓp)R p ∞ N n R 2 Locally Convex ///// L p > 1 L R , C(R ) R pointwise, ℓweak Inner Product ///// L2 ℓ2[0, 1] ///// ///// Locally Compact Rn ///// ///// ///// ///// 1. A set is balanced when λ 6 1 λA A. | | ⇒ ⊆ (a) The image and pre-image of balanced sets are balanced. ◦ (b) The closure and interior are again balanced (if A 0; since λA = (λA)◦ A◦); as are the union, intersection, sum,∈ scaling, T and prod- uct A ⊆B of balanced sets. -
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∗. -
[Math.AG] 10 Jan 2008
FLAGS IN ZERO DIMENSIONAL COMPLETE INTERSECTION ALGEBRAS AND INDICES OF REAL VECTOR FIELDS L. GIRALDO, X. GOMEZ-MONT´ AND P. MARDESIˇ C´ Abstract. We introduce bilinear forms in a flag in a complete intersection local R-algebra of dimension 0, related to the Eisenbud-Levine, Khimshiashvili bilinear form. We give a variational interpretation of these forms in terms of Jantzen’s filtration and bilinear forms. We use the signatures of these forms to compute in the real case the constant relating the GSV-index with the signature function of vector fields tangent to an even dimensional hypersurface singularity, one being topologically defined and the other computable with finite dimensional commutative algebra methods. 0. Introduction n Let f1,...,fn : R → R be germs of real analytic functions that form a regular sequence as holomorphic functions and let ARn A := ,0 (1) (f1,...,fn) be the quotient finite dimensional algebra, where ARn,0 is the algebra of germs of n real analytic functions on R with coordinates x1,...,xn. The class of the Jacobian ∂fi J = det , JA := [J]A ∈ A (2) ∂x j i,j=1,...,n generates the socle (the unique minimal non-zero ideal) of the algebra A. A sym- metric bilinear form · LA arXiv:math/0612275v2 [math.AG] 10 Jan 2008 <,>LA : A × A→A→R (3) is defined by composing multiplication in A with any linear map LA : A −→ R sending JA to a positive number. The theory of Eisenbud-Levine and Khimshi- ashvili asserts that this bilinear form is nondegenerate and that its signature σA is independent of the choice of LA (see [3], [12]). -
Torsion, As a Function on the Space of Representations
TORSION, AS A FUNCTION ON THE SPACE OF REPRESENTATIONS DAN BURGHELEA AND STEFAN HALLER Abstract. For a closed manifold M we introduce the set of co-Euler struc- tures as Poincar´edual of Euler structures. The Riemannian Geometry, Topol- ogy and Dynamics on manifolds permit to introduce partially defined holomor- phic functions on RepM (Γ; V ) called in this paper complex valued Ray{Singer torsion, Milnor{Turaev torsion, and dynamical torsion. They are associated essentially to M plus an Euler (or co-Euler structure) and a Riemannian met- ric plus additional geometric data in the first case, a smooth triangulation in the second case and a smooth flow of type described in section 2 in the third case. In this paper we define these functions, show they are essentially equal and have analytic continuation to rational functions on RepM (Γ; V ), describe some of their properties and calculate them in some case. We also recognize familiar rational functions in topology (Lefschetz zeta function of a diffeomor- phism, dynamical zeta function of closed trajectories, Alexander polynomial of a knot) as particular cases of our torsions. A numerical invariant derived from Ray{Singer torsion and associated to two homotopic acyclic representations is discussed in the last section. Contents 1. Introduction 2 2. Characteristic forms and vector fields 3 3. Euler and co-Euler structures 6 4. Complex representations and cochain complexes 8 5. Analytic torsion 11 6. Milnor{Turaev and dynamical torsion 14 7. Examples 16 8. Applications 17 References 19 Date: August 12, 2005. 2000 Mathematics Subject Classification. 57R20, 58J52. Key words and phrases. -
Chapter IX. Tensors and Multilinear Forms
Notes c F.P. Greenleaf and S. Marques 2006-2016 LAII-s16-quadforms.tex version 4/25/2016 Chapter IX. Tensors and Multilinear Forms. IX.1. Basic Definitions and Examples. 1.1. Definition. A bilinear form is a map B : V V C that is linear in each entry when the other entry is held fixed, so that × → B(αx, y) = αB(x, y)= B(x, αy) B(x + x ,y) = B(x ,y)+ B(x ,y) for all α F, x V, y V 1 2 1 2 ∈ k ∈ k ∈ B(x, y1 + y2) = B(x, y1)+ B(x, y2) (This of course forces B(x, y)=0 if either input is zero.) We say B is symmetric if B(x, y)= B(y, x), for all x, y and antisymmetric if B(x, y)= B(y, x). Similarly a multilinear form (aka a k-linear form , or a tensor− of rank k) is a map B : V V F that is linear in each entry when the other entries are held fixed. ×···×(0,k) → We write V = V ∗ . V ∗ for the set of k-linear forms. The reason we use V ∗ here rather than V , and⊗ the⊗ rationale for the “tensor product” notation, will gradually become clear. The set V ∗ V ∗ of bilinear forms on V becomes a vector space over F if we define ⊗ 1. Zero element: B(x, y) = 0 for all x, y V ; ∈ 2. Scalar multiple: (αB)(x, y)= αB(x, y), for α F and x, y V ; ∈ ∈ 3. Addition: (B + B )(x, y)= B (x, y)+ B (x, y), for x, y V . -
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. -
Jordan Triple Systems with Completely Reducible Derivation Or Structure Algebras
Pacific Journal of Mathematics JORDAN TRIPLE SYSTEMS WITH COMPLETELY REDUCIBLE DERIVATION OR STRUCTURE ALGEBRAS E. NEHER Vol. 113, No. 1 March 1984 PACIFIC JOURNAL OF MATHEMATICS Vol. 113, No. 1,1984 JORDAN TRIPLE SYSTEMS WITH COMPLETELY REDUCIBLE DERIVATION OR STRUCTURE ALGEBRAS ERHARD NEHER We prove that a finite-dimensional Jordan triple system over a field k of characteristic zero has a completely reducible structure algebra iff it is a direct sum of a trivial and a semisimple ideal. This theorem depends on a classification of Jordan triple systems with completely reducible derivation algebra in the case where k is algebraically closed. As another application we characterize real Jordan triple systems with compact automorphism group. The main topic of this paper is finite-dimensional Jordan triple systems over a field of characteristic zero which have a completely reducible derivation algebra. The history of the subject begins with [7] where G. Hochschild proved, among other results, that for an associative algebra & the deriva- tion algebra is semisimple iff & itself is semisimple. Later on R. D. Schafer considered in [18] the case of a Jordan algebra £. His result was that Der f is semisimple if and only if $ is semisimple with each simple component of dimension not equal to 3 over its center. This theorem was extended by K.-H. Helwig, who proved in [6]: Let f be a Jordan algebra which is finite-dimensional over a field of characteristic zero. Then the following are equivlent: (1) Der % is completely reducible and every derivation of % has trace zero, (2) £ is semisimple, (3) the bilinear form on Der f> given by (Dl9 D2) -> trace(Z>!Z>2) is non-degenerate and every derivation of % is inner. -
Complex G2-Manifolds and Seiberg-Witten Equations
Journal of Gökova Geometry Topology Volume 13 (2019) 15 – 40 Complex G2-manifolds and Seiberg-Witten Equations Selman Akbulut and Üstün Yıldırım Abstract. We introduce the notion of complex G2 manifold MC, and complexifica- tion of a G2 manifold M ⊂ MC. As an application we show the following: If (Y; s) is a closed oriented 3-manifold with a Spinc structure, and (Y; s) ⊂ (M; ') is an imbedding as an associative submanifold of some G2 manifold (such imbedding al- ways exists), then the isotropic associative deformations of Y in the complexified G2 manifold MC is given by Seiberg-Witten equations. Contents 1. Introduction 16 2. Linear algebra 17 2.1. Symmetric bilinear forms and S1 family of metrics 18 C 2.2. The group G2 20 2.3. Alternating three-forms in seven-space 24 2.4. The complexification of a G2-space 25 C 2.5. Compatible structures on a G2 -space 26 3. Grassmannians 28 3.1. Associative Grassmannian 28 3.2. Isotropic Grassmannian 30 3.3. Isotropic associative Grassmannian 32 3.4. B-Real associative Grassmannian 32 3.5. Diagram of all Grassmannians 34 C 4. G2 -manifolds 35 5. Complexification of a G2 manifold 36 6. Deforming associative submanifolds in complexification 37 6.1. Deformation as isotropic associative 38 6.2. Deformation as B-real associative 39 References 40 2010 Mathematics Subject Classification. 53C38, 53C29, 57R57. Key words and phrases. G2 manifold, complex G2 manifold, associative submanifold. First named author is partially supported by NSF grant 1505364. 15 AKBULUT and YILDIRIM 1. Introduction 7 An almost G2 manifold (M ;') is a 7-manifold whose tangent frame bundle reduces to the Lie group G2. -
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. -
Arxiv:Math/0601536V2 [Math.AC] 5 Sep 2006 Nt Dimensional; finite Ecl Qaematrix Square a Call We T Hrceitci Eoe by Denoted Is Characteristic Its Notations
Non-degenerate bilinear forms in characteristic 2, related contact forms, simple Lie algebras and superalgebras Alexei Lebedev ∗ Abstract Non-degenerate bilinear forms over fields of characteristic 2, in particular, non- symmetric ones, are classified with respect to various equivalences, and the Lie algebras preserving them are described. Although it is known that there are two series of distinct finite simple Chevalley groups preserving the non-degenerate symmetric bilinear forms on the space of even dimension, the description of simple Lie algebras related to the ones that preserve these forms is new. The classification of 1-forms is shown to be related to one of the considered equivalences of bilinear forms. A version of the above results for superspaces is also given. §1 Introduction 1.1 Notations. The ground field K is assumed to be algebraically closed unless specified; its characteristic is denoted by p; we assume that p = 2 unless specified; vector spaces V are finite dimensional; n = dim V . We often use the following matrices 0 1 k if n =2k, 1k 0 ! 0 1n J2n = , Πn = 0 01 k −1n 0 (1.1) 0 1 0 if n =2k +1, 1k 0 0 arXiv:math/0601536v2 [math.AC] 5 Sep 2006 S(n) = antidiag (1,..., 1), Z(2k) = diag(Π ,..., Π ). n k 2 2 We call a square matrix zero-diagonal if it has only zeros on the main diagonal; let ZD(n) be the space (Lie algebra if p = 2) of symmetric zero-diagonal n × n-matrices. For any Lie (super)algebra g, let g(1) = [g, g] and g(i+1) = [g(i), g(i)].