Conjugacy Classes in Finite Unitary Groups

Total Page:16

File Type:pdf, Size:1020Kb

Conjugacy Classes in Finite Unitary Groups Conjugacy Classes in Finite Unitary Groups D. E. Taylor Version of 26 June, 2021 TEXed: 3 August, 2021 This treatment of the general unitary groups is modelled on the reports ‘Conjugacy Classes in Finite Special and General Linear Groups’ and ‘Conjugacy Classes in Finite Symplectic Groups’. It also uses ideas from the preprint [2] and the C code of Sergei Haller implementing conjugacy classes for the conformal unitary groups (see the file classes_classical.c). The conjugacy classes are obtained by first computing a complete collection of invariants, determining a representative matrix for each invariant and then computing the order of its centraliser directly from the invariant. This construction is based on the work of Wall [4]. 1 Finite unitary groups For a prime power q, let k GF.q2/ and let k k x x denote the automorphism of q D W !n W 7! N n k defined by x x . If f .t/ a0 a1t ant kŒt, let f .t/ a0 a1t ant . N D D C C C 2 DN CN C C N The general unitary group The general unitary group GU.n; q/ considered here is the set of n n matrices A over the tr field k such that AƒA ƒ, where Atr is the transpose of A and ƒ is the ‘standard’ hermitian D form 00 0 0 11 B0 0 1 0C B . C ƒn B .. C : D B C @0 1 0 0A 1 0 0 0 The description of the conjugacy classes of GU.n; q/ closely parallels the description of the conjugacy classes of GL.n; q/ and Sp.2n; q/. The group GU.n; q/ acts on V kn and for g GU.n; q/, the space V becomes a kŒt- D 2 module Vg by defining vf .t/ vf .g/ for all v V and all f .t/ kŒt. The hermitian form D 2 2 on V preserved by GU.n; q/ is defined by ˇ.u; v/ uƒvtr. D The conformal unitary group The conformal unitary group CGU.n; q/ is the group of linear transformations g such that ˇ.ug; vg/ .g/ˇ.u; v/ for some .g/ k and all u; v V . In matrix terms this is equivalent tr D 2 2 to AƒA .g/ƒ. On applying the automorphism we see that .g/ k0, the fixed field D 2 of . 1 If we identify k with the corresponding scalar matrix we have ˇ.u; v/ and 2 D N since the norm map is onto we see that CGU.n; q/ Z GU.n; q/, where Z is the centre of D CGU.n; q/. Therefore, if g1, g2,..., gr represent the conjugacy classes of GU.n; q/, the conjugacy i classes of CGU.n; q/ are represented by the elements gj , where is a primitive element of k, 1 i < q and 1 j r. Thus from now on we restrict our attention to the general unitary Ä Ä Ä group. import “common.m” : centralJoin, convert ; import “Classes/translate/translateU.m” : tagToNameGU, tagToNameSU ; 2 Polynomials and partitions If P is the set of all partitions and ˆ is the set of all monic irreducible polynomials (other than t), then for g GL.n; q2/ there is a function ˆ P such that 2 W ! M i .f / Vg kŒt=.f / (2.1) D f ˆ;i 2 and .f / .1.f /; 2.f /; : : : ; / is a partition such that D X deg.f / .f / n: j j D f ˆ 2 If g GU.n; q/ there are restrictions—to be determined in the sections which follow—on 2 the polynomials that can occur in this decomposition. Polynomials Definition 2.1. (i) Let f .t/ kŒt be a monic polynomial of degree d such that f .0/ 0. The twisted dual 2 ¤ of f .t/ is the polynomial 1 f .t/ f .0/ t d f .t 1/: Q D (ii) The polynomial f .t/ is symmetric if f .t/ f .t/. Q D (iii) A polynomial f .t/ is irreducible if it is symmetric and has no proper symmetric factors. d 1 d The monic polynomial f .t/ a0 a1t ad 1t t is symmetric if and only if D C C C C a0a0 1 and ad i a0ai for 0 < i < d. (2.2) D D It is clear that for monic polynomials f and g we have f f and .fg/ f g. Q D D Q Q intrinsic TILDEDUALPOLYNOMIAL( f :: RNGUPOLELT ) RNGUPOLELT { The twisted dual of the polynomial f !} eseq := COEFFICIENTS(f ); a0 := eseq[1]; e 2 require a0 ne 0 : “Polynomial must have non-zero constant term”; K := COEFFICIENTRING(f ); flag, q := ISSQUARE(#K ); require flag : “Field size must be a square”; cseq := [e q : e in eseq ]; return cseq[1] 1 PARENT(f ) !REVERSE(cseq); end intrinsic; If g preserves the hermitian form ˇ, then for all u; v V we have 2 ˇ.ug; v/ ˇ.u; vg 1/ D and thus for f .t/ kŒt 2 ˇ.uf.g/; v/ ˇ.u; vf .g 1//: (2.3) D In particular, if m.t/ is the minimal polynomial of g, then vm.g 1/ 0 for all v and therefore D gd m.g 1/ 0, where d is the degree of m.t/. Thus m.g/ 0 and it follows that m.t/ m.t/; D Q D Q D that is, the minimal polynomial of g is symmetric. Lemma 2.2. Let f .t/ be a monic irreducible polynomial. (i) If f .t/ is reducible, there exists an irreducible polynomial h.t/ such that f .t/ h.t/h.t/ and D Q h.t/ h.t/. ¤ Q d (ii) If f .t/ is irreducible, the degree d of f .t/ is odd and q 1 1 for all such that f ./ 0. C D D Proof. (i) Suppose that h.t/ is an irreducible factor of f .t/. Then g.t/ divides f .t/ f .t/ and Q Q D since f .t/ is irreducible f .t/ h.t/h.t/ and h.t/ h.t/. D Q Q ¤ (ii) (Ennola [1, Lemma 2]) Let be a root of f and let e be the order of . Then f f D Q implies f . 1/ 0 and so f . q/ 0. The Galois group Gal.kŒ; k/ is generated by D D 2 x xq W 7! q i q2i 2d and therefore ./ for some i such that 0 i < d. Since kŒ q we also 2d D D Ä j j D have q . Thus q2i 1 1 .mod e/ and q2d 1 .mod e/. D Á Á Let s gcd.2i 1; 2d/. There exist integers a and b such that D s a.2i 1/ 2bd D C and it follows that qs qa.2i 1/ 2bd . 1/a .mod e/. But s is odd, hence s divides d and D C Á since a is odd, qs 1 .mod e/. Thus if d is even, qd 1 .mod e/. But then d=2./ , Á Á d D which is a contradiction. Therefore d is odd, qd 1 and so q 1 1. Á C D intrinsic TILDEIRREDUCIBLEPOLYNOMIALS( q :: RNGINTELT, d :: RNGINTELT ) SEQENUM {All monic polynomials of degree d with no proper ! tilde-symmetric factors} K := GF(q 2); P := POLYNOMIALRING(K ); is a generator of the group of field elements of norm 1. (q 1) := PRIMITIVEELEMENT(K ) ; 3 if d eq 1 then return [P P:1 i : i in [0:: q]]; end if; j m := d div 2; if ISEVEN(d ) then pols := (m eq 1) select [P P:1 a : a in K a ne 0 ] j j else ALLIRREDUCIBLEPOLYNOMIALS(K , m); pols := SETSEQ( h hh : h in pols h ne hh where hh is TILDEDUALPOLYNOMIAL(h) ); f j g else // d is odd pols := [P ]; j V := VECTORSPACE(K , m); Construct all symmetric polynomials of degree d. for i := 0 to q do i a0 := ; for v in V do eseq := [a0] cat ELTSEQ(v ); q eseq cat:= [a0 eseq[m+1 j ] : j in [0:: m 1]] cat [K ! 1]; f := P ! eseq ; if ISIRREDUCIBLE(f ) then APPEND( pols, f ); end if; end for; end for; end if; return pols ; end intrinsic; Conjugacy class invariants Proof We shall see that elements g1; g2 GU.n; q/ are conjugate in GU.n; q/ if and only if 2 required! they are conjugate in GL.n; q2/ and the conjugacy classes in GU.n; q/ are parametrised by sequences Œ f; f ˆ;e P , where ˆe is the set of irreducible polynomials. h i j 2 2 The class invariants can be constructed in several steps. Firstly, choose a partition D Œn1; n2; : : : ; nk of d. If has m parts of size n, choose m polynomials of degree n (with repetition) represented as a list of pairs, where f; r indicates that the polynomial f of h i degree n has been chosen r times. Secondly, refine by replacing each pair f; r by f; , where is a partition of r. This h i h i refinement step is carried out by the following function. refine := function() ƒ := [ @@ ]; f g for in do := []; f , r := EXPLODE(); for in PARTITIONS(r ) do ˇ := convert (); for in ƒ do APPEND( ,INCLUDE(, <f , ˇ> )); end for; end for; ƒ := ; end for; 4 return ƒ ; end function; intrinsic INTERNALCLASSINVARIANTSGU( d :: RNGINTELT, q :: RNGINTELT : SUBSET := “All”) SEQENUM {The! sequence of conjugacy class invariants for the general unitary group GU(d,q)} if SUBSET eq “Unipotent” then t := POLYNOMIALRING(GF(q 2)):1; return [ @ <t 1, convert (part )> @ : part in PARTITIONS(d )]; f g end if; pols := [TILDEIRREDUCIBLEPOLYNOMIALS(q, k ): k in [1:: d ]]; polsz := [ 1::#pols[k ] : k in [1:: d ]]; f g ptnz := [convert (): in PARTITIONS(d )]; inv := []; for ı in ptnz do prev := [ @@ ]; f g for term in ı do ss := []; n, m := EXPLODE(term); pp := pols[n]; for S in MULTISETS(polsz[n], m) do if SUBSET eq “Semisimple” then „ := [ @@ ]; f g for i r in S do ! „ := [ INCLUDE(, <pp[i ], [<1, r >]>): in „]; end for; else := [ < pp[i ], r > : i r in S ]; ! „ := refine(); end if; for stub in prev do for in „ do APPEND( ss, stub join ); end for; end for; end for; prev := ss ; end for; inv cat:= ss ; end for; return inv ; end intrinsic; Given the sequence pif of primary invariant factors f; m of a unitary matrix, for each h i polynomial f combine the multiplicities m into a partition and replace f by f f if f f .
Recommended publications
  • Lecture Notes: Qubit Representations and Rotations
    Phys 711 Topics in Particles & Fields | Spring 2013 | Lecture 1 | v0.3 Lecture notes: Qubit representations and rotations Jeffrey Yepez Department of Physics and Astronomy University of Hawai`i at Manoa Watanabe Hall, 2505 Correa Road Honolulu, Hawai`i 96822 E-mail: [email protected] www.phys.hawaii.edu/∼yepez (Dated: January 9, 2013) Contents mathematical object (an abstraction of a two-state quan- tum object) with a \one" state and a \zero" state: I. What is a qubit? 1 1 0 II. Time-dependent qubits states 2 jqi = αj0i + βj1i = α + β ; (1) 0 1 III. Qubit representations 2 A. Hilbert space representation 2 where α and β are complex numbers. These complex B. SU(2) and O(3) representations 2 numbers are called amplitudes. The basis states are or- IV. Rotation by similarity transformation 3 thonormal V. Rotation transformation in exponential form 5 h0j0i = h1j1i = 1 (2a) VI. Composition of qubit rotations 7 h0j1i = h1j0i = 0: (2b) A. Special case of equal angles 7 In general, the qubit jqi in (1) is said to be in a superpo- VII. Example composite rotation 7 sition state of the two logical basis states j0i and j1i. If References 9 α and β are complex, it would seem that a qubit should have four free real-valued parameters (two magnitudes and two phases): I. WHAT IS A QUBIT? iθ0 α φ0 e jqi = = iθ1 : (3) Let us begin by introducing some notation: β φ1 e 1 state (called \minus" on the Bloch sphere) Yet, for a qubit to contain only one classical bit of infor- 0 mation, the qubit need only be unimodular (normalized j1i = the alternate symbol is |−i 1 to unity) α∗α + β∗β = 1: (4) 0 state (called \plus" on the Bloch sphere) 1 Hence it lives on the complex unit circle, depicted on the j0i = the alternate symbol is j+i: 0 top of Figure 1.
    [Show full text]
  • Field Theory 1. Introduction to Quantum Field Theory (A Primer for a Basic Education)
    Field Theory 1. Introduction to Quantum Field Theory (A Primer for a Basic Education) Roberto Soldati February 23, 2019 Contents 0.1 Prologue ............................ 4 1 Basics in Group Theory 8 1.1 Groups and Group Representations . 8 1.1.1 Definitions ....................... 8 1.1.2 Theorems ........................ 12 1.1.3 Direct Products of Group Representations . 14 1.2 Continuous Groups and Lie Groups . 16 1.2.1 The Continuous Groups . 16 1.2.2 The Lie Groups .................... 18 1.2.3 An Example : the Rotations Group . 19 1.2.4 The Infinitesimal Operators . 21 1.2.5 Lie Algebra ....................... 23 1.2.6 The Exponential Representation . 24 1.2.7 The Special Unitary Groups . 27 1.3 The Non-Homogeneous Lorentz Group . 34 1.3.1 The Lorentz Group . 34 1.3.2 Semi-Simple Groups . 43 1.3.3 The Poincar´eGroup . 49 2 The Action Functional 57 2.1 The Classical Relativistic Wave Fields . 57 2.1.1 Field Variations .................... 58 2.1.2 The Scalar and Vector Fields . 62 2.1.3 The Spinor Fields ................... 65 2.2 The Action Principle ................... 76 2.3 The N¨otherTheorem ................... 79 2.3.1 Problems ........................ 87 1 3 The Scalar Field 94 3.1 General Features ...................... 94 3.2 Normal Modes Expansion . 101 3.3 Klein-Gordon Quantum Field . 106 3.4 The Fock Space .......................112 3.4.1 The Many-Particle States . 112 3.4.2 The Lorentz Covariance Properties . 116 3.5 Special Distributions . 129 3.5.1 Euclidean Formulation . 133 3.6 Problems ............................137 4 The Spinor Field 151 4.1 The Dirac Equation .
    [Show full text]
  • Unitary Group - Wikipedia
    Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group Unitary group In mathematics, the unitary group of degree n, denoted U( n), is the group of n × n unitary matrices, with the group operation of matrix multiplication. The unitary group is a subgroup of the general linear group GL( n, C). Hyperorthogonal group is an archaic name for the unitary group, especially over finite fields. For the group of unitary matrices with determinant 1, see Special unitary group. In the simple case n = 1, the group U(1) corresponds to the circle group, consisting of all complex numbers with absolute value 1 under multiplication. All the unitary groups contain copies of this group. The unitary group U( n) is a real Lie group of dimension n2. The Lie algebra of U( n) consists of n × n skew-Hermitian matrices, with the Lie bracket given by the commutator. The general unitary group (also called the group of unitary similitudes ) consists of all matrices A such that A∗A is a nonzero multiple of the identity matrix, and is just the product of the unitary group with the group of all positive multiples of the identity matrix. Contents Properties Topology Related groups 2-out-of-3 property Special unitary and projective unitary groups G-structure: almost Hermitian Generalizations Indefinite forms Finite fields Degree-2 separable algebras Algebraic groups Unitary group of a quadratic module Polynomial invariants Classifying space See also Notes References Properties Since the determinant of a unitary matrix is a complex number with norm 1, the determinant gives a group 1 of 7 2/23/2018, 10:13 AM Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group homomorphism The kernel of this homomorphism is the set of unitary matrices with determinant 1.
    [Show full text]
  • Parametrization of 3×3 Unitary Matrices Based on Polarization
    Parametrization of 33 unitary matrices based on polarization algebra (May, 2018) José J. Gil Parametrization of 33 unitary matrices based on polarization algebra José J. Gil Universidad de Zaragoza. Pedro Cerbuna 12, 50009 Zaragoza Spain [email protected] Abstract A parametrization of 33 unitary matrices is presented. This mathematical approach is inspired by polarization algebra and is formulated through the identification of a set of three orthonormal three-dimensional Jones vectors representing respective pure polarization states. This approach leads to the representation of a 33 unitary matrix as an orthogonal similarity transformation of a particular type of unitary matrix that depends on six independent parameters, while the remaining three parameters correspond to the orthogonal matrix of the said transformation. The results obtained are applied to determine the structure of the second component of the characteristic decomposition of a 33 positive semidefinite Hermitian matrix. 1 Introduction In many branches of Mathematics, Physics and Engineering, 33 unitary matrices appear as key elements for solving a great variety of problems, and therefore, appropriate parameterizations in terms of minimum sets of nine independent parameters are required for the corresponding mathematical treatment. In this way, some interesting parametrizations have been obtained [1-8]. In particular, the Cabibbo-Kobayashi-Maskawa matrix (CKM matrix) [6,7], which represents information on the strength of flavour-changing weak decays and depends on four parameters, constitutes the core of a family of parametrizations of a 33 unitary matrix [8]. In this paper, a new general parametrization is presented, which is inspired by polarization algebra [9] through the structure of orthonormal sets of three-dimensional Jones vectors [10].
    [Show full text]
  • Matrix Lie Groups
    Maths Seminar 2007 MATRIX LIE GROUPS Claudiu C Remsing Dept of Mathematics (Pure and Applied) Rhodes University Grahamstown 6140 26 September 2007 RhodesUniv CCR 0 Maths Seminar 2007 TALK OUTLINE 1. What is a matrix Lie group ? 2. Matrices revisited. 3. Examples of matrix Lie groups. 4. Matrix Lie algebras. 5. A glimpse at elementary Lie theory. 6. Life beyond elementary Lie theory. RhodesUniv CCR 1 Maths Seminar 2007 1. What is a matrix Lie group ? Matrix Lie groups are groups of invertible • matrices that have desirable geometric features. So matrix Lie groups are simultaneously algebraic and geometric objects. Matrix Lie groups naturally arise in • – geometry (classical, algebraic, differential) – complex analyis – differential equations – Fourier analysis – algebra (group theory, ring theory) – number theory – combinatorics. RhodesUniv CCR 2 Maths Seminar 2007 Matrix Lie groups are encountered in many • applications in – physics (geometric mechanics, quantum con- trol) – engineering (motion control, robotics) – computational chemistry (molecular mo- tion) – computer science (computer animation, computer vision, quantum computation). “It turns out that matrix [Lie] groups • pop up in virtually any investigation of objects with symmetries, such as molecules in chemistry, particles in physics, and projective spaces in geometry”. (K. Tapp, 2005) RhodesUniv CCR 3 Maths Seminar 2007 EXAMPLE 1 : The Euclidean group E (2). • E (2) = F : R2 R2 F is an isometry . → | n o The vector space R2 is equipped with the standard Euclidean structure (the “dot product”) x y = x y + x y (x, y R2), • 1 1 2 2 ∈ hence with the Euclidean distance d (x, y) = (y x) (y x) (x, y R2).
    [Show full text]
  • The Classical Groups and Domains 1. the Disk, Upper Half-Plane, SL 2(R
    (June 8, 2018) The Classical Groups and Domains Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ The complex unit disk D = fz 2 C : jzj < 1g has four families of generalizations to bounded open subsets in Cn with groups acting transitively upon them. Such domains, defined more precisely below, are bounded symmetric domains. First, we recall some standard facts about the unit disk, the upper half-plane, the ambient complex projective line, and corresponding groups acting by linear fractional (M¨obius)transformations. Happily, many of the higher- dimensional bounded symmetric domains behave in a manner that is a simple extension of this simplest case. 1. The disk, upper half-plane, SL2(R), and U(1; 1) 2. Classical groups over C and over R 3. The four families of self-adjoint cones 4. The four families of classical domains 5. Harish-Chandra's and Borel's realization of domains 1. The disk, upper half-plane, SL2(R), and U(1; 1) The group a b GL ( ) = f : a; b; c; d 2 ; ad − bc 6= 0g 2 C c d C acts on the extended complex plane C [ 1 by linear fractional transformations a b az + b (z) = c d cz + d with the traditional natural convention about arithmetic with 1. But we can be more precise, in a form helpful for higher-dimensional cases: introduce homogeneous coordinates for the complex projective line P1, by defining P1 to be a set of cosets u 1 = f : not both u; v are 0g= × = 2 − f0g = × P v C C C where C× acts by scalar multiplication.
    [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]
  • 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]
  • Bott Periodicity for the Unitary Group
    Bott Periodicity for the Unitary Group Carlos Salinas March 7, 2018 Abstract We will present a condensed proof of the Bott Periodicity Theorem for the unitary group U following John Milnor’s classic Morse Theory. There are many documents on the internet which already purport to do this (and do so very well in my estimation), but I nevertheless will attempt to give a summary of the result. Contents 1 The Basics 2 2 Fiber Bundles 3 2.1 First fiber bundle . .4 2.2 Second Fiber Bundle . .5 2.3 Third Fiber Bundle . .5 2.4 Fourth Fiber Bundle . .5 3 Proof of the Periodicity Theorem 6 3.1 The first equivalence . .7 3.2 The second equality . .8 4 The Homotopy Groups of U 8 1 The Basics The original proof of the Periodicity Theorem relies on a deep result of Marston Morse’s calculus of variations, the (Morse) Index Theorem. The proof of this theorem, however, goes beyond the scope of this document, the reader is welcome to read the relevant section from Milnor or indeed Morse’s own paper titled The Index Theorem in the Calculus of Variations. Perhaps the first thing we should set about doing is introducing the main character of our story; this will be the unitary group. The unitary group of degree n (here denoted U(n)) is the set of all unitary matrices; that is, the set of all A ∈ GL(n, C) such that AA∗ = I where A∗ is the conjugate of the transpose of A (conjugate transpose for short).
    [Show full text]
  • Extending Symmetries of the Standard Model Towards Grand Unification
    Master research Extending Symmetries of the Standard Model towards Grand Unification Anno Touwen Supervisor prof. dr. Dani¨el Boer August 3, 2018 Abstract In this master thesis the spacetime, global and gauge symmetries of the Standard Model are reviewed. These symmetries are used as a basis for finding possible extensions of this successful model, such as the two Higgs doublet model and Left-Right model. Methods of finding subgroups and the slitting up of representations are discussed based on Dynkin diagrams. These methods are applied to analyse the subgroups of the exceptional group E6 as candidates for Grand Unified 3 Theory groups. In this study SU(5), SO(10) and SU(3) and SU(4)×SU(2)×SU(2) are most important. A phenomenological comparison between these models is given focussed on the different types of leptoquarks that could be responsible for the not yet observed proton decay. Contents 1 Introduction 3 2 Symmetry groups and Gauge theories 5 2.1 Group theory . .5 2.2 Unitary and Special Unitary groups . .8 2.3 Orthogonal and Special Orthogonal groups . 10 2.4 Gauge theories and fields . 11 2.5 Spacetime symmetries . 13 2.6 C, P and T transformations . 14 3 The Standard Model 16 3.1 The Electroweak interaction . 16 3.2 The Strong interaction . 19 3.3 Fermion content . 19 3.4 Eigenstates and the CKM-matrix . 22 3.5 Global symmetries . 23 4 Beyond the Standard Model 28 4.1 Two Higgs doublet model . 28 4.2 Left-Right models . 34 5 A further study of Lie Groups and Algebras 37 5.1 Root systems .
    [Show full text]
  • Math 408 Advanced Linear Algebra Chi-Kwong Li Chapter 2 Unitary
    Math 408 Advanced Linear Algebra Chi-Kwong Li Chapter 2 Unitary similarity and normal matrices n ∗ Definition A set of vector fx1; : : : ; xkg in C is orthogonal if xi xj = 0 for i 6= j. If, in addition, ∗ that xj xj = 1 for each j, then the set is orthonormal. Theorem An orthonormal set of vectors in Cn is linearly independent. n Definition An orthonormal set fx1; : : : ; xng in C is an orthonormal basis. A matrix U 2 Mn ∗ is unitary if it has orthonormal columns, i.e., U U = In. Theorem Let U 2 Mn. The following are equivalent. (a) U is unitary. (b) U is invertible and U ∗ = U −1. ∗ ∗ (c) UU = In, i.e., U is unitary. (d) kUxk = kxk for all x 2 Cn, where kxk = (x∗x)1=2. Remarks (1) Real unitary matrices are orthogonal matrices. (2) Unitary (real orthogonal) matrices form a group in the set of complex (real) matrices and is a subgroup of the group of invertible matrices. ∗ Definition Two matrices A; B 2 Mn are unitarily similar if A = U BU for some unitary U. Theorem If A; B 2 Mn are unitarily similar, then X 2 ∗ ∗ X 2 jaijj = tr (A A) = tr (B B) = jbijj : i;j i;j Specht's Theorem Two matrices A and B are similar if and only if tr W (A; A∗) = tr W (B; B∗) for all words of length of degree at most 2n2. Schur's Theorem Every A 2 Mn is unitarily similar to a upper triangular matrix. Theorem Every A 2 Mn(R) is orthogonally similar to a matrix in upper triangular block form so that the diagonal blocks have size at most 2.
    [Show full text]
  • Representation Theory
    M392C NOTES: REPRESENTATION THEORY ARUN DEBRAY MAY 14, 2017 These notes were taken in UT Austin's M392C (Representation Theory) class in Spring 2017, taught by Sam Gunningham. I live-TEXed them using vim, so there may be typos; please send questions, comments, complaints, and corrections to [email protected]. Thanks to Kartik Chitturi, Adrian Clough, Tom Gannon, Nathan Guermond, Sam Gunningham, Jay Hathaway, and Surya Raghavendran for correcting a few errors. Contents 1. Lie groups and smooth actions: 1/18/172 2. Representation theory of compact groups: 1/20/174 3. Operations on representations: 1/23/176 4. Complete reducibility: 1/25/178 5. Some examples: 1/27/17 10 6. Matrix coefficients and characters: 1/30/17 12 7. The Peter-Weyl theorem: 2/1/17 13 8. Character tables: 2/3/17 15 9. The character theory of SU(2): 2/6/17 17 10. Representation theory of Lie groups: 2/8/17 19 11. Lie algebras: 2/10/17 20 12. The adjoint representations: 2/13/17 22 13. Representations of Lie algebras: 2/15/17 24 14. The representation theory of sl2(C): 2/17/17 25 15. Solvable and nilpotent Lie algebras: 2/20/17 27 16. Semisimple Lie algebras: 2/22/17 29 17. Invariant bilinear forms on Lie algebras: 2/24/17 31 18. Classical Lie groups and Lie algebras: 2/27/17 32 19. Roots and root spaces: 3/1/17 34 20. Properties of roots: 3/3/17 36 21. Root systems: 3/6/17 37 22. Dynkin diagrams: 3/8/17 39 23.
    [Show full text]