DOCSLIB.ORG

SL2(R) and FRACTIONAL LINEAR TRANSFORMATION General Linear

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
SL2(R) and FRACTIONAL LINEAR TRANSFORMATION General Linear SL2(R) AND FRACTIONAL LINEAR TRANSFORMATION general linear group and projective line For a general field F general linear group is a a b GL ( ) = : ad − bc 6= 0 2 F c d 2 The action of GL2(F) on F is the matrix multiplication of 2 × 2−matrices with 1 × 2−matrices. The special linear group is an a b SL ( ) = : ad − bc = 1 2 F c d Definition 1. (a; b) 2 F2 is called an admissible pair if there exists c; d 2 F such a b that 2 GL ( ): c d 2 F Definition 2. we define an equivalence relation on F2 nf(0; 0)g as follows: (x; y) ∼ (u; v) if there is a non-zero λ 2 F such that x = λu and y = λv: Definition 3. P(F) = f[x : y]:(x; y) is admissibleg is called the projective line over F: The projective line over F is the extension of a usual line by a point called a point at infinity. Mobius¨ transformation A linear map F2 ! F2 is a class invariant for ∼: Thereby, the linear transforma- tion of F2 produces the map P(F) ! P(F) as follows: a b [x : y] = [ax + by : cx + dy]; ad − bc 6= 0; c d where a; b; c; d 2 F: a b Definition 4. For some A = 2 SL ( ): The map T :( ) ! ( ) is c d 2 F A F F defined by TA([x : y]) = [ax + by : cx + dy]:TA is called a M¨obiustransformation. Proposition 5. the set of all M¨obiustransformations is isomorphic to SL2(F)={∓Ig Lemma 6. TA([u]) = [u] if and only if u is an eigenvector of A: The eigenvectors of A (the fixed points of TA) is [x : y] = [(a − d) ± p(d + a)2 − 4 : 2c]: Then we can classify M¨obiusmaps through eigenvalues of A: If F = R or C then Date: October 15, 2017. 1 (1) A has two different complex-conjugated eigenvalues if and only if 0 ≤ tr2(g) < 4: That means, g fixes two distinct complex-conjugated points in P(C) and fixes no point in P(R): Such a map is called elliptic. (2) A has a double eigenvalue if and only if tr2(g) = 4: That means, g fixes a double point. Such a map is called parabolic. (3) A has two distinct real eigenvalues if and only if tr2(g) > 4: That means, g fixes two distinct points. Such a map is called hyperbolic. (4) For K = C; there is an extra class as follows. A has two distinct non-real eigenvalues if and only if tr2(g) 2= [0; 1): In other words, A has two distinct complex eigenvalues if Im(ptr2(g)) 6= 0: That means, g fixes two distinct complex points. Such a map is called strictly loxodromic. The last type of transformation is not possible for K = R: The class, which contains the classes of hyperbolic and strictly loxodromic maps, is called the class of loxodromic maps. Proposition 7. Let TA be a M¨obiustransformation and suppose TA leaves three points fixed. Then TA is the identity map. Proposition 8. Fix w0; w − 1; w2 distinct. Then, for each distinct z0; z1; z2, there is exactly one TA with TA(wi) = zi; for i = 0; 1; 2: w1−w2 w−w0 Let f(w) = : f(w0) = 0; f(w1) = 1; f(w2) = 1: w1−w0 w−w2 one-parameter subgroup Based on the number of fixed points, there are only, up to similarity and rescal- ing, the following three types of non-trivial one-parameter subgroups of SL2(R) . cosh t sinh t 1 0 cos t − sin t A(t) = ;N(t) = and K(t) = : sinh t cosh t t 1 sin t cos t a b Let H = : a; b 2 : Every element in H fixes [1 : 0]: 0 1 R Let p : SL2(R) ! P(R) be a function defined by p(g) = [b : d] where g = a b : c d Let s : P(R) ! SL2(R) be a function defined by: 8 ! > 1 x > if x 2 R; <> 0 1 s(x) = ! > 0 −1 > if x = 1: :> 1 0 The third important map here is r : SL2(R) ! H which is defined by: s(p(g))r(g) = g: Therefore the action of SL2(R) on P(R) is g : x ! p(g ∗ s(x)): The action of SL2(R) on the projective line is a M¨obiustransformation. The action of SL2(R) on the upper half plane (unit disk) is equivalent to Cayley transform which is given 1 −i by C = : −i 1 2 double and dual numbers The commutative ring with identity of all double numbers is the triple (O; +; ·); where O = fo = a + bj : a; b 2 Rg; and for all a = a1 + a2j; b = b1 + b2j in O addition and multiplication are defined as follows: (1) a + b = (a1 + a2j) + (b1 + b2j) = (a1 + b1) + (a2 + b2)j: (2) a · b = (a1 + a2j) · (b1 + b2j) = (a1b1 + a2b2) + (a2b1 + a1b2)j: In particular j2 = 1. The commutative ring with identity of all dual numbers is the triple (D; +; ·); where D = fd = a + b : a; b 2 Rg; and for all a = a1 + a2, b = b1 + b2 in D addition and multiplication are defined as follows: (1) a + b = (a1 + a2) + (b1 + b2) = (a1 + b1) + (a2 + b2). (2) a · b = (a1 + a2) · (b1 + b2) = a1b1 + (a2b1 + a1b2). 2 In particular = 0: Let A be one of O; D: GL2(A) is the set of all invertible 2×2−matrices. SL2(A) is the set of all invertible 2×2−matrices with determinant equal to 1. P(O) = O [ f1; σ1; σ2g [ fa!1; a!2 : a 2 Rg: P(D) = D [ f1; a! : a 2 Rg: References [1] Alan F. Beardon, The geometry of discrete groups, Graduate Texts in Mathematics, vol. 91, Springer-Verlag, New York, 1995. Corrected reprint of the 1983 original. MR1393195 [2] Vladimir V. Kisil, Geometry of M¨obiustransformations, Imperial College Press, London, 2012. Elliptic, parabolic and hyperbolic actions of SL2(R), With 1 DVD-ROM. MR2977041 [3] Barry Simon, Szeg¨o'stheorem and its descendants, M. B. Porter Lectures, Princeton Univer- sity Press, Princeton, NJ, 2011. Spectral theory for L2 perturbations of orthogonal polyno- mials. MR2743058 3.
Load more

Recommended publications
  • Low-Dimensional Representations of Matrix Groups and Group Actions on CAT (0) Spaces and Manifolds
    Low-dimensional representations of matrix groups and group actions on CAT(0) spaces and manifolds Shengkui Ye National University of Singapore January 8, 2018 Abstract We study low-dimensional representations of matrix groups over gen- eral rings, by considering group actions on CAT(0) spaces, spheres and acyclic manifolds. 1 Introduction Low-dimensional representations are studied by many authors, such as Gural- nick and Tiep [24] (for matrix groups over fields), Potapchik and Rapinchuk [30] (for automorphism group of free group), Dokovi´cand Platonov [18] (for Aut(F2)), Weinberger [35] (for SLn(Z)) and so on. In this article, we study low-dimensional representations of matrix groups over general rings. Let R be an associative ring with identity and En(R) (n ≥ 3) the group generated by ele- mentary matrices (cf. Section 3.1). As motivation, we can consider the following problem. Problem 1. For n ≥ 3, is there any nontrivial group homomorphism En(R) → En−1(R)? arXiv:1207.6747v1 [math.GT] 29 Jul 2012 Although this is a purely algebraic problem, in general it seems hard to give an answer in an algebraic way. In this article, we try to answer Prob- lem 1 negatively from the point of view of geometric group theory. The idea is to find a good geometric object on which En−1(R) acts naturally and non- trivially while En(R) can only act in a special way. We study matrix group actions on CAT(0) spaces, spheres and acyclic manifolds. We prove that for low-dimensional CAT(0) spaces, a matrix group action always has a global fixed point (cf.
    [Show full text]
  • The General Linear Group
    18.704 Gabe Cunningham 2/18/05 [email protected] The General Linear Group Definition: Let F be a field. Then the general linear group GLn(F ) is the group of invert- ible n × n matrices with entries in F under matrix multiplication. It is easy to see that GLn(F ) is, in fact, a group: matrix multiplication is associative; the identity element is In, the n × n matrix with 1’s along the main diagonal and 0’s everywhere else; and the matrices are invertible by choice. It’s not immediately clear whether GLn(F ) has infinitely many elements when F does. However, such is the case. Let a ∈ F , a 6= 0. −1 Then a · In is an invertible n × n matrix with inverse a · In. In fact, the set of all such × matrices forms a subgroup of GLn(F ) that is isomorphic to F = F \{0}. It is clear that if F is a finite field, then GLn(F ) has only finitely many elements. An interesting question to ask is how many elements it has. Before addressing that question fully, let’s look at some examples. ∼ × Example 1: Let n = 1. Then GLn(Fq) = Fq , which has q − 1 elements. a b Example 2: Let n = 2; let M = ( c d ). Then for M to be invertible, it is necessary and sufficient that ad 6= bc. If a, b, c, and d are all nonzero, then we can fix a, b, and c arbitrarily, and d can be anything but a−1bc. This gives us (q − 1)3(q − 2) matrices.
    [Show full text]
  • Lie Group and Geometry on the Lie Group SL2(R)
    INDIAN INSTITUTE OF TECHNOLOGY KHARAGPUR Lie group and Geometry on the Lie Group SL2(R) PROJECT REPORT – SEMESTER IV MOUSUMI MALICK 2-YEARS MSc(2011-2012) Guided by –Prof.DEBAPRIYA BISWAS Lie group and Geometry on the Lie Group SL2(R) CERTIFICATE This is to certify that the project entitled “Lie group and Geometry on the Lie group SL2(R)” being submitted by Mousumi Malick Roll no.-10MA40017, Department of Mathematics is a survey of some beautiful results in Lie groups and its geometry and this has been carried out under my supervision. Dr. Debapriya Biswas Department of Mathematics Date- Indian Institute of Technology Khargpur 1 Lie group and Geometry on the Lie Group SL2(R) ACKNOWLEDGEMENT I wish to express my gratitude to Dr. Debapriya Biswas for her help and guidance in preparing this project. Thanks are also due to the other professor of this department for their constant encouragement. Date- place-IIT Kharagpur Mousumi Malick 2 Lie group and Geometry on the Lie Group SL2(R) CONTENTS 1.Introduction ................................................................................................... 4 2.Definition of general linear group: ............................................................... 5 3.Definition of a general Lie group:................................................................... 5 4.Definition of group action: ............................................................................. 5 5. Definition of orbit under a group action: ...................................................... 5 6.1.The general linear
    [Show full text]
  • GEOMETRY and GROUPS These Notes Are to Remind You of The
    GEOMETRY AND GROUPS These notes are to remind you of the results from earlier courses that we will need at some point in this course. The exercises are entirely optional, although they will all be useful later in the course. Asterisks indicate that they are harder. 0.1 Metric Spaces (Metric and Topological Spaces) A metric on a set X is a map d : X × X → [0, ∞) that satisfies: (a) d(x, y) > 0 with equality if and only if x = y; (b) Symmetry: d(x, y) = d(y, x) for all x, y ∈ X; (c) Triangle Rule: d(x, y) + d(y, z) > d(x, z) for all x, y, z ∈ X. A set X with a metric d is called a metric space. For example, the Euclidean metric on RN is given by d(x, y) = ||x − y|| where v u N ! u X 2 ||a|| = t |an| n=1 is the norm of a vector a. This metric makes RN into a metric space and any subset of it is also a metric space. A sequence in X is a map N → X; n 7→ xn. We often denote this sequence by (xn). This sequence converges to a limit ` ∈ X when d(xn, `) → 0 as n → ∞ . A subsequence of the sequence (xn) is given by taking only some of the terms in the sequence. So, a subsequence of the sequence (xn) is given by n 7→ xk(n) where k : N → N is a strictly increasing function. A metric space X is (sequentially) compact if every sequence from X has a subsequence that converges to a point of X.
    [Show full text]
  • 10 Group Theory
    10 Group theory 10.1 What is a group? A group G is a set of elements f, g, h, ... and an operation called multipli- cation such that for all elements f,g, and h in the group G: 1. The product fg is in the group G (closure); 2. f(gh)=(fg)h (associativity); 3. there is an identity element e in the group G such that ge = eg = g; 1 1 1 4. every g in G has an inverse g− in G such that gg− = g− g = e. Physical transformations naturally form groups. The elements of a group might be all physical transformations on a given set of objects that leave invariant a chosen property of the set of objects. For instance, the objects might be the points (x, y) in a plane. The chosen property could be their distances x2 + y2 from the origin. The physical transformations that leave unchanged these distances are the rotations about the origin p x cos ✓ sin ✓ x 0 = . (10.1) y sin ✓ cos ✓ y ✓ 0◆ ✓− ◆✓ ◆ These rotations form the special orthogonal group in 2 dimensions, SO(2). More generally, suppose the transformations T,T0,T00,... change a set of objects in ways that leave invariant a chosen property property of the objects. Suppose the product T 0 T of the transformations T and T 0 represents the action of T followed by the action of T 0 on the objects. Since both T and T 0 leave the chosen property unchanged, so will their product T 0 T . Thus the closure condition is satisfied.
    [Show full text]
  • Matrix Lie Groups and Their Lie Algebras
    Matrix Lie groups and their Lie algebras Alen Alexanderian∗ Abstract We discuss matrix Lie groups and their corresponding Lie algebras. Some common examples are provided for purpose of illustration. 1 Introduction The goal of these brief note is to provide a quick introduction to matrix Lie groups which are a special class of abstract Lie groups. Study of matrix Lie groups is a fruitful endeavor which allows one an entry to theory of Lie groups without requiring knowl- edge of differential topology. After all, most interesting Lie groups turn out to be matrix groups anyway. An abstract Lie group is defined to be a group which is also a smooth manifold, where the group operations of multiplication and inversion are also smooth. We provide a much simple definition for a matrix Lie group in Section 4. Showing that a matrix Lie group is in fact a Lie group is discussed in standard texts such as [2]. We also discuss Lie algebras [1], and the computation of the Lie algebra of a Lie group in Section 5. We will compute the Lie algebras of several well known Lie groups in that section for the purpose of illustration. 2 Notation Let V be a vector space. We denote by gl(V) the space of all linear transformations on V. If V is a finite-dimensional vector space we may put an arbitrary basis on V and identify elements of gl(V) with their matrix representation. The following define various classes of matrices on Rn: ∗The University of Texas at Austin, USA. E-mail: [email protected] Last revised: July 12, 2013 Matrix Lie groups gl(n) : the space of n
    [Show full text]
  • 1 the Spin Homomorphism SL2(C) → SO1,3(R) a Summary from Multiple Sources Written by Y
    1 The spin homomorphism SL2(C) ! SO1;3(R) A summary from multiple sources written by Y. Feng and Katherine E. Stange Abstract We will discuss the spin homomorphism SL2(C) ! SO1;3(R) in three manners. Firstly we interpret SL2(C) as acting on the Minkowski 1;3 spacetime R ; secondly by viewing the quadratic form as a twisted 1 1 P × P ; and finally using Clifford groups. 1.1 Introduction The spin homomorphism SL2(C) ! SO1;3(R) is a homomorphism of classical matrix Lie groups. The lefthand group con- sists of 2 × 2 complex matrices with determinant 1. The righthand group consists of 4 × 4 real matrices with determinant 1 which preserve some fixed real quadratic form Q of signature (1; 3). This map is alternately called the spinor map and variations. The image of this map is the identity component + of SO1;3(R), denoted SO1;3(R). The kernel is {±Ig. Therefore, we obtain an isomorphism + PSL2(C) = SL2(C)= ± I ' SO1;3(R): This is one of a family of isomorphisms of Lie groups called exceptional iso- morphisms. In Section 1.3, we give the spin homomorphism explicitly, al- though these formulae are unenlightening by themselves. In Section 1.4 we describe O1;3(R) in greater detail as the group of Lorentz transformations. This document describes this homomorphism from three distinct per- spectives. The first is very concrete, and constructs, using the language of Minkowski space, Lorentz transformations and Hermitian matrices, an ex- 4 plicit action of SL2(C) on R preserving Q (Section 1.5).
    [Show full text]
  • A STUDY on the ALGEBRAIC STRUCTURE of SL 2(Zpz)
    A STUDY ON THE ALGEBRAIC STRUCTURE OF SL2 Z pZ ( ~ ) A Thesis Presented to The Honors Tutorial College Ohio University In Partial Fulfillment of the Requirements for Graduation from the Honors Tutorial College with the degree of Bachelor of Science in Mathematics by Evan North April 2015 Contents 1 Introduction 1 2 Background 5 2.1 Group Theory . 5 2.2 Linear Algebra . 14 2.3 Matrix Group SL2 R Over a Ring . 22 ( ) 3 Conjugacy Classes of Matrix Groups 26 3.1 Order of the Matrix Groups . 26 3.2 Conjugacy Classes of GL2 Fp ....................... 28 3.2.1 Linear Case . .( . .) . 29 3.2.2 First Quadratic Case . 29 3.2.3 Second Quadratic Case . 30 3.2.4 Third Quadratic Case . 31 3.2.5 Classes in SL2 Fp ......................... 33 3.3 Splitting of Classes of(SL)2 Fp ....................... 35 3.4 Results of SL2 Fp ..............................( ) 40 ( ) 2 4 Toward Lifting to SL2 Z p Z 41 4.1 Reduction mod p ...............................( ~ ) 42 4.2 Exploring the Kernel . 43 i 4.3 Generalizing to SL2 Z p Z ........................ 46 ( ~ ) 5 Closing Remarks 48 5.1 Future Work . 48 5.2 Conclusion . 48 1 Introduction Symmetries are one of the most widely-known examples of pure mathematics. Symmetry is when an object can be rotated, flipped, or otherwise transformed in such a way that its appearance remains the same. Basic geometric figures should create familiar examples, take for instance the triangle. Figure 1: The symmetries of a triangle: 3 reflections, 2 rotations. The red lines represent the reflection symmetries, where the trianlge is flipped over, while the arrows represent the rotational symmetry of the triangle.
    [Show full text]
  • 1 Classical Groups (Problems Sets 1 – 5)
    1 Classical Groups (Problems Sets 1 { 5) De¯nitions. A nonempty set G together with an operation ¤ is a group provided ² The set is closed under the operation. That is, if g and h belong to the set G, then so does g ¤ h. ² The operation is associative. That is, if g; h and k are any elements of G, then g ¤ (h ¤ k) = (g ¤ h) ¤ k. ² There is an element e of G which is an identity for the operation. That is, if g is any element of G, then g ¤ e = e ¤ g = g. ² Every element of G has an inverse in G. That is, if g is in G then there is an element of G denoted g¡1 so that g ¤ g¡1 = g¡1 ¤ g = e. The group G is abelian if g ¤ h = h ¤ g for all g; h 2 G. A nonempty subset H ⊆ G is a subgroup of the group G if H is itself a group with the same operation ¤ as G. That is, H is a subgroup provided ² H is closed under the operation. ² H contains the identity e. ² Every element of H has an inverse in H. 1.1 Groups of symmetries. Symmetries are invertible functions from some set to itself preserving some feature of the set (shape, distance, interval, :::). A set of symmetries of a set can form a group using the operation composition of functions. If f and g are functions from a set X to itself, then the composition of f and g is denoted f ± g, and it is de¯ned by (f ± g)(x) = f(g(x)) for x in X.
    [Show full text]
  • Matrices Lie: an Introduction to Matrix Lie Groups and Matrix Lie Algebras
    Matrices Lie: An introduction to matrix Lie groups and matrix Lie algebras By Max Lloyd A Journal submitted in partial fulfillment of the requirements for graduation in Mathematics. Abstract: This paper is an introduction to Lie theory and matrix Lie groups. In working with familiar transformations on real, complex and quaternion vector spaces this paper will define many well studied matrix Lie groups and their associated Lie algebras. In doing so it will introduce the types of vectors being transformed, types of transformations, what groups of these transformations look like, tangent spaces of specific groups and the structure of their Lie algebras. Whitman College 2015 1 Contents 1 Acknowledgments 3 2 Introduction 3 3 Types of Numbers and Their Representations 3 3.1 Real (R)................................4 3.2 Complex (C).............................4 3.3 Quaternion (H)............................5 4 Transformations and General Geometric Groups 8 4.1 Linear Transformations . .8 4.2 Geometric Matrix Groups . .9 4.3 Defining SO(2)............................9 5 Conditions for Matrix Elements of General Geometric Groups 11 5.1 SO(n) and O(n)........................... 11 5.2 U(n) and SU(n)........................... 14 5.3 Sp(n)................................. 16 6 Tangent Spaces and Lie Algebras 18 6.1 Introductions . 18 6.1.1 Tangent Space of SO(2) . 18 6.1.2 Formal Definition of the Tangent Space . 18 6.1.3 Tangent space of Sp(1) and introduction to Lie Algebras . 19 6.2 Tangent Vectors of O(n), U(n) and Sp(n)............. 21 6.3 Tangent Space and Lie algebra of SO(n).............. 22 6.4 Tangent Space and Lie algebras of U(n), SU(n) and Sp(n)..
    [Show full text]
  • A Linear Algebraic Group? Skip Garibaldi
    WHATIS... ? a Linear Algebraic Group? Skip Garibaldi From a marketing perspective, algebraic groups group over F, a Lie group, or a topological group is are poorly named.They are not the groups you met a “group object” in the category of affine varieties as a student in abstract algebra, which I will call over F, smooth manifolds, or topological spaces, concrete groups for clarity. Rather, an algebraic respectively. For algebraic groups, this implies group is the analogue in algebra of a topological that the set G(K) is a concrete group for each field group (fromtopology) or a Liegroup (from analysis K containing F. and geometry). Algebraic groups provide a unifying language Examples for apparently different results in algebra and The basic example is the general linear group number theory. This unification can not only sim- GLn for which GLn(K) is the concrete group of plify proofs, it can also suggest generalizations invertible n-by-n matrices with entries in K. It is the and bring new tools to bear, such as Galois co- collection of solutions (t, X)—with t ∈ K and X an homology, Steenrod operations in Chow theory, n-by-n matrix over K—to the polynomial equation etc. t ·det X = 1. Similar reasoning shows that familiar matrix groups such as SLn, orthogonal groups, Definitions and symplectic groups can be viewed as linear A linear algebraic group over a field F is a smooth algebraic groups. The main difference here is that affine variety over F that is also a group, much instead of viewing them as collections of matrices like a topological group is a topological space over F, we view them as collections of matrices that is also a group and a Lie group is a smooth over every extension K of F.
    [Show full text]
  • 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.
    [Show full text]