Hints and Solutions to Selected Exercises

Total Page:16

File Type:pdf, Size:1020Kb

Hints and Solutions to Selected Exercises Hints and Solutions to Selected Exercises Chapter 1 1.1. Using the formula of Remark 1.4, we obtain II[~ ~]II = J2IUI2+1~J4IUI2+1, II [~ ~] II = max{lul, Ivl}, C?S t - sin t] II = 1 cosh t sinh t] II = {t -t} II [smt cost ' II [sinh t cosh t max e ,e . 1.2. (a) From the definition of the matrix norm, -1 { IBAB-Ixl }{ IAxl } IIBAB II = max Ixl :x t 0 = max IBxl: x t 0 = max {I~~I :x to} = IIAII. (b) The inequality IICAC- I II ~ IICIlIIAIIIIC- I II always holds. 1.3. (a) We have Ixl 2 = x·x by definition, so Since the unit sphere {x E en : Ixl = 1} is closed and bounded, the continuous 2 function x I---> IAxl defined on it attains its supremum, hence 2 (b) The matrix A*A is hermitian and for any x E en, x*A*Ax = IAxI , which is real and non-negative; it also vanishes precisely when Ax = O. By the general theory of hermitian matrices, there is an orthonormal basis {UI, ... ,Un} consisting of eigenvalues AI, ... ,An which are all real. For each j, 303 304 Matrix Groups: An Introduction to Lie Group Theory since ujUj = 1; hence Aj ~ O. If A i= 0 there must be at least one non-zero eigenvalue of A*A since otherwise IAxl2 would always vanish; so in this case we have a largest positive eigenvalue A which we might as well assume is A= AI. Now if Ixl = 1 we can 2 2 write x = tIU1 + ... + tnun, where tj EC and ItII + ... + Itn l = 1. Then 2 x* A*Ax = X*(A1tIU1 + ... + AntnUn) = A11tl12 + + An ltnl ~ A11tII 2 + + A11tnl2 = A1, hence IIAII 2 ~ Al and in fact we have equality since uiA*AU1 = AI. 1.4. (a) Let 1 ( . IIAr+111) £ = 2 1 + r~~ lA::lI < 1. For large enough m we have IIAm + ... + Am+kll ~ IIAmll + ... + II Am+k1l m m m m Am = IIAmll (1 + IIA +l1l + IIA +dIIlA +211 + ... + IIA +lll .. 'II +kll) II Am II IIAmIiIlAm+l1l IIAmll" ·IIAm+k-111 < IIAmll (1 + £ + £2 + ... + £k-l) = II Am II \11-=-£;1-+ I~A_m~1 as k -+ 00. Also, if mo is large enough, then for m > mo, II~:~~ II < £, so IIAmll = ::~:~~il·.I!~~:::IIIAmoll < £m-mOIiAmoll-+ 0 as m -+ 00. Combining these we see that the partial sums of the series form a Cauchy sequence and hence the series converges. (b) Here IIAml1 -+ 00 as m -+ 00 and the series diverges. (c) Any of the usual tests based on absolute convergence works. 1.5. (a) For m, n ~ 1, m m m m n II~ Arll = IIA + Am+! + ... + Am+nll ~ IIAli + IIAll +! + ... + IIAli + A n 1 = IIAli m (1 _II ll + ) -+ 0 as m n -+ 00 (1 -IIAII) ,. So the sequence of partial sums is a Cauchy sequence. This can also be done using the ratio test of Exercise 1.4. (b) For any n ~ 1, (I - A)(I + A + A 2 + ... + An) = 1- An+ 1 = (I + A + A 2 + ... + An)(I - A), so 2 n 1 n II (I - A)(I + A + A + ... + An) - III = IIA + 11 ~ IiAli +l -+ 0 as n -+ 00, and similarly for II(I + A + A 2 + ... + An)(I - A) - III. Hence I - A has inverse 00 r (I - A)-l = LA . r=O Hints and Solutions to Selected Exercises 305 (c) If A k = 0, then k-1 k-1 (I - A)-l = LAr, exp(A) = L ~Ar. T. r=O r=O 1.6. (a) The subset O(n) = {A E Mn(R) : ATA - I = O} ~ Mn(R) is bounded since for A E O(n), IIAII = 1. It is also closed since if a sequence Ar E O(n) converges to A EMn(R) then ATA - I = lim (A;Ar - 1) = lim 0 = O. r-+CX) r-+oo Therefore O(n) is compact. (b) The subset U(n) = {A E Mn(C) : A*A - I = O} ~ Mn(C) is compact by a similar argument to (a). (c) Consider the n x n diagonal matrices A k = diag(k, 11k, 1, ... ,1) (k ~ 1). Then detAk = 1 so Ak E SLn(k) ~ GLn(k). But IIAkll = k -+ 00 as k -+ 00, so this sequence is unbounded. 1.7. (a) If A, BE H then there are sequences Ar ,Br in H with Ar -+ A and Br -+ B as T -+ 00. Hence ArBr -+ AB and so AB E H since each ArBr E H. Similarly, A;:-l -+ A-I, showing that A-I E H. (b) Here is an alternative proof in terms of open sets which applies to any topological group. Let u, v E H and consider uv. If uv f/. H, the open set G - H contains uv; notice that G - H is the biggest open subset of G which does not intersect H. Since the product map mult is continuous, there is an open set of the form U x V ~ G x G contained in the open set mult-1(G - H) with u E U and v E V. Notice that UnH = 0 = vnH by the above remark. Now take u' E UnH and v' E VnH and note that u'v' = mult(u', v') E H and also mult(u', v') E G - H, giving a contradiction. So uv E H. Also, if wE H, suppose that w-1 E G -H. Then inv-1(G -H) ~ G is open, where inv is the inverse map. But as w E inv-1 (G - H), there must be an element hE H n inv-1 (G - H) and so h-1 E G - H which is impossible. Hence H ~ G. (c) Consider any sequence of diagonal matrices A k = diag(ak' 1, ... ,1) (k ~ 1) where ak ~ 1 and ak -+ v'2 as k -+ 00 (v'2 could be replaced by any other irrational number greater than 1). Then Ak -+ diag(v'2, 1, ... ,1) f/. r. We must have r = GLn(lR) since for every B = [bij] E GLn(lR) we can find sequences b~7) E Q satisfying b~7) -+ bij as k -+ 00. 1.8. By Proposition 1.26, G ~ Mn(k) is a closed subset of GLn(lR). 1.9. Suppose that G ~ GLn(lR) ~ Mn(lR) for some n. Then H ~ Mn(lR) is closed and bounded since G is compact. For each h E H the set {h} ~ H is open and these form 306 Matrix Groups: An Introduction to Lie Group Theory an open cover of H by disjoint open sets. By the Hein~Borel Theorem 1.20 there must be finitely many of these sets that cover H, so H is itself finite. 1.10. In each case, we have subgroups Gn+l ~ GLn+l(k) (where k = R or C) and Gn ~ GLn(k) where Gn+! is closed in GLn+l(k) and Gn = Gn+l n GLn(k). As GLn(k) is closed in GLn+l(k), Gn is closed in Gn +!. 1.11. (a) If A E SymP2m(R), then ATJ2mA = J2m and as detJ2m = 1, we have detA2 = 1, so detA = ±1. (b) Let A = [~ ~] E SymP2(R). By definition, [~ ~][_~ ~][~ ~]=[_adO+bC adobc]=[_~ ~], so A E SymP2(R) if and only if detA = Ii hence Symp2(R) ~ SL2(R). 1.12. Clearly Pn U(n) ~ pn GLn(C). If Z = [Zr.] E Mn(C) where Zr. = Xr• +Yr.i with Xr.,Yr. E R, then Pn(Z·) = Pn([X.r] - [Y.riJ) = Pn(Z)T. Hence Z E U(n) if and only if Pn(Z) E O(2n). If A E O(2n), then A E SymP2n(R.) if and only if Ahn = hnA and by Proposition 1.44 this is equivalent to A E pn U(n). This shows that pn U(n) = O(2n)nSymP2n(R).1f BE Symp2n(JR) then Bhn = hnB T if and only if B = B. This shows that pn GLn(C)nSymP2n(R) = O(2n)nSymP2n(R). The second collection of equalities is proved in a similar way. 1.13. (a) The triangle inequality for P follows from the following sequence of inequal­ ities valid for any (XI,X2), (YI,Y2), (ZI,Z2) E Xl X X2, P((XI, X2), (Zl, Z2)) =JPI (Xl, ZI)2 + P2(X2, Z2)2 ~J(PI(XI' YI) + PI(YI, zdF + (p2(X2, Y2) + P2(Y2, Z2))2 [by the triangle inequalities for PI and P2] [by the usual triangle inequality for R2] The other properties required for p to be a metric are straightforward to check. If UI x U2 ~ Xl X X2 with UI ~ Xl and U2 ~ X2 open, then for each Xl E UI and X2 E U2 there are open discs NX1>Pl(Xlirl) ~ UI and NX2,P2(X2ir2) ~ U2i for r = min{rl,r2}, we have NX1XX2,P((XI,x2)jr) ~ UI x U2, so UI X U2 is open with respect to p. Conversely, for an open disc NX1XX2,P((XI,x2);r) we have NX1,Pl(xl;r/v'2) x NX2,P2 (X2i r/v'2) ~ NX1XX2'P((XI,x2)jr). Hence every subset of Xl x X2 open with respect to P is a union of products of open discs in Xl and X 2 • So the topology associated with p has the same open sets as the product topology. (b) If (XI,r,X2,r) -. (XI,X2) say, then for i = 1,2, Pi(Xi,r, Xi) ~ P((XI,r,X2,r), (XI,X2)), Hints and Solutions to Selected Exercises 307 SO Xi,r .....
Recommended publications
  • Groups and Geometry 2018 Auckland University Projective Planes
    Groups and Geometry 2018 Auckland University Projective planes, Laguerre planes and generalized quadrangles that admit large groups of automorphisms G¨unterSteinke School of Mathematics and Statistics University of Canterbury 24 January 2018 G¨unterSteinke Projective planes, Laguerre planes, generalized quadrangles GaG2018 1 / 26 (School of Mathematics and Statistics University of Canterbury) Projective and affine planes Definition A projective plane P = (P; L) consists of a set P of points and a set L of lines (where lines are subsets of P) such that the following three axioms are satisfied: (J) Two distinct points can be joined by a unique line. (I) Two distinct lines intersect in precisely one point. (R) There are at least four points no three of which are on a line. Removing a line and all of its points from a projective plane yields an affine plane. Conversely, each affine plane extends to a unique projective plane by adjoining in each line with an `ideal' point and adding a new line of all ideal points. G¨unterSteinke Projective planes, Laguerre planes, generalized quadrangles GaG2018 2 / 26 (School of Mathematics and Statistics University of Canterbury) Models of projective planes Desarguesian projective planes are obtained from a 3-dimensional vector space V over a skewfield F. Points are the 1-dimensional vector subspaces of V and lines are the 2-dimensional vector subspaces of V . In case F is a field one obtains the Pappian projective plane over F. There are many non-Desarguesian projective planes. One of the earliest and very important class is obtain by the (generalized) Moulton planes.
    [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]
  • Generalisations of the Fundamental Theorem of Projective
    GENERALIZATIONS OF THE FUNDAMENTAL THEOREM OF PROJECTIVE GEOMETRY A thesis submitted for the degree of Doctor of Philosophy By Rupert McCallum Supervisor: Professor Michael Cowling School of Mathematics, The University of New South Wales. March 2009 Acknowledgements I would particularly like to thank my supervisor, Professor Michael Cowling, for conceiving of the research project and providing much valuable feedback and guidance, and providing help with writing the Extended Abstract. I would like to thank the University of New South Wales and the School of Mathematics and Statistics for their financial support. I would like to thank Dr Adam Harris for giving me helpful feedback on drafts of the thesis, and particularly my uncle Professor William McCallum for providing me with detailed comments on many preliminary drafts. I would like to thank Professor Michael Eastwood for making an important contribution to the research project and discussing some of the issues with me. I would like to thank Dr Jason Jeffers and Professor Alan Beardon for helping me with research about the history of the topic. I would like to thank Dr Henri Jimbo for reading over an early draft of the thesis and providing useful suggestions for taking the research further. I would like to thank Dr David Ullrich for drawing my attention to the theorem that if A is a subset of a locally compact Abelian group of positive Haar measure, then A+A has nonempty interior, which was crucial for the results of Chapter 8. I am very grateful to my parents for all the support and encouragement they gave me during the writing of this thesis.
    [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]
  • 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]
  • Arxiv:1009.4249V12 [Math.MG] 17 Oct 2012 H Dniyof Identity the a K Ulig Fsmsml Leri Ruswihetbihsti.W O P Now We This
    A LOCAL-TO-GLOBAL RESULT FOR TOPOLOGICAL SPHERICAL BUILDINGS RUPERT McCALLUM Abstract. Suppose that ∆, ∆′ are two buildings each arising from a semisimple algebraic group over a field, a topological field in the former case, and that for both the buildings the Coxeter diagram has no isolated nodes. We give conditions under which a partially defined injective chamber map, whose domain is the subcomplex of ∆ generated by a nonempty open set of chambers, and whose codomain is ∆′, is guaranteed to extend to a unique injective chamber map. Related to this result is a local version of the Borel-Tits theorem on abstract homomorphisms of simple algebraic groups. Keywords: topological geometry, local homomorphism, topological building, Borel-Tits the- orem Mathematicsl Subject Classification 2000: 51H10 1. Introduction Throughout the history of Lie theory there has been a notion of “local isomorphism”. Indeed, the original notion of Lie groups considered by Sophus Lie in [9] was an essentially local one. Suppose that G is an algebraic group defined over a Hausdorff topological field k. One may consider the notion of a local k-isogeny from the group G to a group G′ defined over k of the same dimension. This is a mapping defined on a nonempty open neighbourhood of the identity of G(k) in the strong k-topology, (see Definition 1.10), which “locally” acts as a k-isogeny, in the sense that it is a local k-homomorphism and its range is Zariski dense. As far as I know this notion has not been investigated systematically. In this paper we shall produce a local version of the Borel-Tits theorem which hints at the possibility that it may be fruitful to investigate this notion.
    [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]
  • Chapter 1 GENERAL STRUCTURE and PROPERTIES
    Chapter 1 GENERAL STRUCTURE AND PROPERTIES 1.1 Introduction In this Chapter we would like to introduce the main de¯nitions and describe the main properties of groups, providing examples to illustrate them. The detailed discussion of representations is however demanded to later Chapters, and so is the treatment of Lie groups based on their relation with Lie algebras. We would also like to introduce several explicit groups, or classes of groups, which are often encountered in Physics (and not only). On the one hand, these \applications" should motivate the more abstract study of the general properties of groups; on the other hand, the knowledge of the more important and common explicit instances of groups is essential for developing an e®ective understanding of the subject beyond the purely formal level. 1.2 Some basic de¯nitions In this Section we give some essential de¯nitions, illustrating them with simple examples. 1.2.1 De¯nition of a group A group G is a set equipped with a binary operation , the group product, such that1 ¢ (i) the group product is associative, namely a; b; c G ; a (b c) = (a b) c ; (1.2.1) 8 2 ¢ ¢ ¢ ¢ (ii) there is in G an identity element e: e G such that a e = e a = a a G ; (1.2.2) 9 2 ¢ ¢ 8 2 (iii) each element a admits an inverse, which is usually denoted as a¡1: a G a¡1 G such that a a¡1 = a¡1 a = e : (1.2.3) 8 2 9 2 ¢ ¢ 1 Notice that the axioms (ii) and (iii) above are in fact redundant.
    [Show full text]
  • COMPACT LIE GROUPS Contents 1. Smooth Manifolds and Maps 1 2
    COMPACT LIE GROUPS NICHOLAS ROUSE Abstract. The first half of the paper presents the basic definitions and results necessary for investigating Lie groups. The primary examples come from the matrix groups. The second half deals with representation theory of groups, particularly compact groups. The end result is the Peter-Weyl theorem. Contents 1. Smooth Manifolds and Maps 1 2. Tangents, Differentials, and Submersions 3 3. Lie Groups 5 4. Group Representations 8 5. Haar Measure and Applications 9 6. The Peter-Weyl Theorem and Consequences 10 Acknowledgments 14 References 14 1. Smooth Manifolds and Maps Manifolds are spaces that, in a certain technical sense defined below, look like Euclidean space. Definition 1.1. A topological manifold of dimension n is a topological space X satisfying: (1) X is second-countable. That is, for the space's topology T , there exists a countable base, which is a countable collection of open sets fBαg in X such that every set in T is the union of a subcollection of fBαg. (2) X is a Hausdorff space. That is, for every pair of points x; y 2 X, there exist open subsets U; V ⊆ X such that x 2 U, y 2 V , and U \ V = ?. (3) X is locally homeomorphic to open subsets of Rn. That is, for every point x 2 X, there exists a neighborhood U ⊆ X of x such that there exists a continuous bijection with a continuous inverse (i.e. a homeomorphism) from U to an open subset of Rn. The first two conditions preclude pathological spaces that happen to have a homeomorphism into Euclidean space, and force a topological manifold to share more properties with Euclidean space.
    [Show full text]