Math 55A: Studies in Algebra and Group Theory
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Arithmetic Equivalence and Isospectrality
ARITHMETIC EQUIVALENCE AND ISOSPECTRALITY ANDREW V.SUTHERLAND ABSTRACT. In these lecture notes we give an introduction to the theory of arithmetic equivalence, a notion originally introduced in a number theoretic setting to refer to number fields with the same zeta function. Gassmann established a direct relationship between arithmetic equivalence and a purely group theoretic notion of equivalence that has since been exploited in several other areas of mathematics, most notably in the spectral theory of Riemannian manifolds by Sunada. We will explicate these results and discuss some applications and generalizations. 1. AN INTRODUCTION TO ARITHMETIC EQUIVALENCE AND ISOSPECTRALITY Let K be a number field (a finite extension of Q), and let OK be its ring of integers (the integral closure of Z in K). The Dedekind zeta function of K is defined by the Dirichlet series X s Y s 1 ζK (s) := N(I)− = (1 N(p)− )− I OK p − ⊆ where the sum ranges over nonzero OK -ideals, the product ranges over nonzero prime ideals, and N(I) := [OK : I] is the absolute norm. For K = Q the Dedekind zeta function ζQ(s) is simply the : P s Riemann zeta function ζ(s) = n 1 n− . As with the Riemann zeta function, the Dirichlet series (and corresponding Euler product) defining≥ the Dedekind zeta function converges absolutely and uniformly to a nonzero holomorphic function on Re(s) > 1, and ζK (s) extends to a meromorphic function on C and satisfies a functional equation, as shown by Hecke [25]. The Dedekind zeta function encodes many features of the number field K: it has a simple pole at s = 1 whose residue is intimately related to several invariants of K, including its class number, and as with the Riemann zeta function, the zeros of ζK (s) are intimately related to the distribution of prime ideals in OK . -
NOTES on FINITE GROUP REPRESENTATIONS in Fall 2020, I
NOTES ON FINITE GROUP REPRESENTATIONS CHARLES REZK In Fall 2020, I taught an undergraduate course on abstract algebra. I chose to spend two weeks on the theory of complex representations of finite groups. I covered the basic concepts, leading to the classification of representations by characters. I also briefly addressed a few more advanced topics, notably induced representations and Frobenius divisibility. I'm making the lectures and these associated notes for this material publicly available. The material here is standard, and is mainly based on Steinberg, Representation theory of finite groups, Ch 2-4, whose notation I will mostly follow. I also used Serre, Linear representations of finite groups, Ch 1-3.1 1. Group representations Given a vector space V over a field F , we write GL(V ) for the group of bijective linear maps T : V ! V . n n When V = F we can write GLn(F ) = GL(F ), and identify the group with the group of invertible n × n matrices. A representation of a group G is a homomorphism of groups φ: G ! GL(V ) for some representation choice of vector space V . I'll usually write φg 2 GL(V ) for the value of φ on g 2 G. n When V = F , so we have a homomorphism φ: G ! GLn(F ), we call it a matrix representation. matrix representation The choice of field F matters. For now, we will look exclusively at the case of F = C, i.e., representations in complex vector spaces. Remark. Since R ⊆ C is a subfield, GLn(R) is a subgroup of GLn(C). -
Class Numbers of Totally Real Number Fields
CLASS NUMBERS OF TOTALLY REAL NUMBER FIELDS BY JOHN C. MILLER A dissertation submitted to the Graduate School|New Brunswick Rutgers, The State University of New Jersey in partial fulfillment of the requirements for the degree of Doctor of Philosophy Graduate Program in Mathematics Written under the direction of Henryk Iwaniec and approved by New Brunswick, New Jersey May, 2015 ABSTRACT OF THE DISSERTATION Class numbers of totally real number fields by John C. Miller Dissertation Director: Henryk Iwaniec The determination of the class number of totally real fields of large discriminant is known to be a difficult problem. The Minkowski bound is too large to be useful, and the root discriminant of the field can be too large to be treated by Odlyzko's discriminant bounds. This thesis describes a new approach. By finding nontrivial lower bounds for sums over prime ideals of the Hilbert class field, we establish upper bounds for class numbers of fields of larger discriminant. This analytic upper bound, together with algebraic arguments concerning the divisibility properties of class numbers, allows us to determine the class numbers of many number fields that have previously been untreatable by any known method. For example, we consider the cyclotomic fields and their real subfields. Surprisingly, the class numbers of cyclotomic fields have only been determined for fields of small conductor, e.g. for prime conductors up to 67, due to the problem of finding the class number of its maximal real subfield, a problem first considered by Kummer. Our results have significantly improved the situation. We also study the cyclotomic Zp-extensions of the rationals. -
Chapter 1 BASICS of GROUP REPRESENTATIONS
Chapter 1 BASICS OF GROUP REPRESENTATIONS 1.1 Group representations A linear representation of a group G is identi¯ed by a module, that is by a couple (D; V ) ; (1.1.1) where V is a vector space, over a ¯eld that for us will always be R or C, called the carrier space, and D is an homomorphism from G to D(G) GL (V ), where GL(V ) is the space of invertible linear operators on V , see Fig. ??. Thus, we ha½ve a is a map g G D(g) GL(V ) ; (1.1.2) 8 2 7! 2 with the linear operators D(g) : v V D(g)v V (1.1.3) 2 7! 2 satisfying the properties D(g1g2) = D(g1)D(g2) ; D(g¡1 = [D(g)]¡1 ; D(e) = 1 : (1.1.4) The product (and the inverse) on the righ hand sides above are those appropriate for operators: D(g1)D(g2) corresponds to acting by D(g2) after having appplied D(g1). In the last line, 1 is the identity operator. We can consider both ¯nite and in¯nite-dimensional carrier spaces. In in¯nite-dimensional spaces, typically spaces of functions, linear operators will typically be linear di®erential operators. Example Consider the in¯nite-dimensional space of in¯nitely-derivable functions (\functions of class 1") Ã(x) de¯ned on R. Consider the group of translations by real numbers: x x + a, C 7! with a R. This group is evidently isomorphic to R; +. As we discussed in sec ??, these transformations2 induce an action D(a) on the functions Ã(x), de¯ned by the requirement that the transformed function in the translated point x + a equals the old original function in the point x, namely, that D(a)Ã(x) = Ã(x a) : (1.1.5) ¡ 1 Group representations 2 It follows that the translation group admits an in¯nite-dimensional representation over the space V of 1 functions given by the di®erential operators C d d a2 d2 D(a) = exp a = 1 a + + : : : : (1.1.6) ¡ dx ¡ dx 2 dx2 µ ¶ In fact, we have d a2 d2 dà a2 d2à D(a)Ã(x) = 1 a + + : : : Ã(x) = Ã(x) a (x) + (x) + : : : = Ã(x a) : ¡ dx 2 dx2 ¡ dx 2 dx2 ¡ · ¸ (1.1.7) In most of this chapter we will however be concerned with ¯nite-dimensional representations. -
REPRESENTATION THEORY WEEK 7 1. Characters of GL Kand Sn A
REPRESENTATION THEORY WEEK 7 1. Characters of GLk and Sn A character of an irreducible representation of GLk is a polynomial function con- stant on every conjugacy class. Since the set of diagonalizable matrices is dense in GLk, a character is defined by its values on the subgroup of diagonal matrices in GLk. Thus, one can consider a character as a polynomial function of x1,...,xk. Moreover, a character is a symmetric polynomial of x1,...,xk as the matrices diag (x1,...,xk) and diag xs(1),...,xs(k) are conjugate for any s ∈ Sk. For example, the character of the standard representation in E is equal to x1 + ⊗n n ··· + xk and the character of E is equal to (x1 + ··· + xk) . Let λ = (λ1,...,λk) be such that λ1 ≥ λ2 ≥ ···≥ λk ≥ 0. Let Dλ denote the λj determinant of the k × k-matrix whose i, j entry equals xi . It is clear that Dλ is a skew-symmetric polynomial of x1,...,xk. If ρ = (k − 1,..., 1, 0) then Dρ = i≤j (xi − xj) is the well known Vandermonde determinant. Let Q Dλ+ρ Sλ = . Dρ It is easy to see that Sλ is a symmetric polynomial of x1,...,xk. It is called a Schur λ1 λk polynomial. The leading monomial of Sλ is the x ...xk (if one orders monomials lexicographically) and therefore it is not hard to show that Sλ form a basis in the ring of symmetric polynomials of x1,...,xk. Theorem 1.1. The character of Wλ equals to Sλ. I do not include a proof of this Theorem since it uses beautiful but hard combina- toric. -
Problem 1 Show That If Π Is an Irreducible Representation of a Compact Lie Group G Then Π∨ Is Also Irreducible
Problem 1 Show that if π is an irreducible representation of a compact lie group G then π_ is also irreducible. Give an example of a G and π such that π =∼ π_, and another for which π π_. Is this true for general groups? R 2 Since G is a compact Lie group, we can apply Schur orthogonality to see that G jχπ_ (g)j dg = R 2 R 2 _ G jχπ(g)j dg = G jχπ(g)j dg = 1, so π is irreducible. For any G, the trivial representation π _ i i satisfies π ' π . For G the cyclic group of order 3 generated by g, the representation π : g 7! ζ3 _ i −i is not isomorphic to π : g 7! ζ3 . This is true for finite dimensional irreducible representations. This follows as if W ⊆ V a proper, non-zero G-invariant representation for a group G, then W ? = fφ 2 V ∗jφ(W ) = 0g is a proper, non-zero G-invariant subspace and applying this to V ∗ as V ∗∗ =∼ V we get V is irreducible if and only if V ∗ is irreducible. This is false for general representations and general groups. Take G = S1 to be the symmetric group on countably infinitely many letters, and let G act on a vector space V over C with basis e1; e2; ··· by sending σ : ei 7! eσ(i). Let W be the sub-representation given by the kernel of the map P P V ! C sending λiei 7! λi. Then W is irreducible because given any λ1e1 + ··· + λnen 2 V −1 where λn 6= 0, and we see that λn [(n n + 1) − 1] 2 C[G] sends this to en+1 − en, and elements like ∗ ∗ this span W . -
Extending Real-Valued Characters of Finite General Linear and Unitary Groups on Elements Related to Regular Unipotents
EXTENDING REAL-VALUED CHARACTERS OF FINITE GENERAL LINEAR AND UNITARY GROUPS ON ELEMENTS RELATED TO REGULAR UNIPOTENTS ROD GOW AND C. RYAN VINROOT Abstract. Let GL(n; Fq)hτi and U(n; Fq2 )hτi denote the finite general linear and unitary groups extended by the transpose inverse automorphism, respec- tively, where q is a power of p. Let n be odd, and let χ be an irreducible character of either of these groups which is an extension of a real-valued char- acter of GL(n; Fq) or U(n; Fq2 ). Let yτ be an element of GL(n; Fq)hτi or 2 U(n; Fq2 )hτi such that (yτ) is regular unipotent in GL(n; Fq) or U(n; Fq2 ), respectively. We show that χ(yτ) = ±1 if χ(1) is prime to p and χ(yτ) = 0 oth- erwise. Several intermediate results on real conjugacy classes and real-valued characters of these groups are obtained along the way. 1. Introduction Let F be a field and let n be a positive integer. Let GL(n; F) denote the general linear group of degree n over F. In the special case that F is the finite field of order q, we denote the corresponding general linear group by GL(n; Fq). Let τ denote the involutory automorphism of GL(n; F) which maps an element g to its transpose inverse (g0)−1, where g0 denotes the transpose of g, and let GL(n; F)hτi denote the semidirect product of GL(n; F) by τ. Thus in GL(n; F)hτi, we have τ 2 = 1 and τgτ = (g0)−1 for g 2 GL(n; F). -
Math 123—Algebra II
Math 123|Algebra II Lectures by Joe Harris Notes by Max Wang Harvard University, Spring 2012 Lecture 1: 1/23/12 . 1 Lecture 19: 3/7/12 . 26 Lecture 2: 1/25/12 . 2 Lecture 21: 3/19/12 . 27 Lecture 3: 1/27/12 . 3 Lecture 22: 3/21/12 . 31 Lecture 4: 1/30/12 . 4 Lecture 23: 3/23/12 . 33 Lecture 5: 2/1/12 . 6 Lecture 24: 3/26/12 . 34 Lecture 6: 2/3/12 . 8 Lecture 25: 3/28/12 . 36 Lecture 7: 2/6/12 . 9 Lecture 26: 3/30/12 . 37 Lecture 8: 2/8/12 . 10 Lecture 27: 4/2/12 . 38 Lecture 9: 2/10/12 . 12 Lecture 28: 4/4/12 . 40 Lecture 10: 2/13/12 . 13 Lecture 29: 4/6/12 . 41 Lecture 11: 2/15/12 . 15 Lecture 30: 4/9/12 . 42 Lecture 12: 2/17/16 . 17 Lecture 31: 4/11/12 . 44 Lecture 13: 2/22/12 . 19 Lecture 14: 2/24/12 . 21 Lecture 32: 4/13/12 . 45 Lecture 15: 2/27/12 . 22 Lecture 33: 4/16/12 . 46 Lecture 17: 3/2/12 . 23 Lecture 34: 4/18/12 . 47 Lecture 18: 3/5/12 . 25 Lecture 35: 4/20/12 . 48 Introduction Math 123 is the second in a two-course undergraduate series on abstract algebra offered at Harvard University. This instance of the course dealt with fields and Galois theory, representation theory of finite groups, and rings and modules. These notes were live-TEXed, then edited for correctness and clarity. -
Math 263A Notes: Algebraic Combinatorics and Symmetric Functions
MATH 263A NOTES: ALGEBRAIC COMBINATORICS AND SYMMETRIC FUNCTIONS AARON LANDESMAN CONTENTS 1. Introduction 4 2. 10/26/16 5 2.1. Logistics 5 2.2. Overview 5 2.3. Down to Math 5 2.4. Partitions 6 2.5. Partial Orders 7 2.6. Monomial Symmetric Functions 7 2.7. Elementary symmetric functions 8 2.8. Course Outline 8 3. 9/28/16 9 3.1. Elementary symmetric functions eλ 9 3.2. Homogeneous symmetric functions, hλ 10 3.3. Power sums pλ 12 4. 9/30/16 14 5. 10/3/16 20 5.1. Expected Number of Fixed Points 20 5.2. Random Matrix Groups 22 5.3. Schur Functions 23 6. 10/5/16 24 6.1. Review 24 6.2. Schur Basis 24 6.3. Hall Inner product 27 7. 10/7/16 29 7.1. Basic properties of the Cauchy product 29 7.2. Discussion of the Cauchy product and related formulas 30 8. 10/10/16 32 8.1. Finishing up last class 32 8.2. Skew-Schur Functions 33 8.3. Jacobi-Trudi 36 9. 10/12/16 37 1 2 AARON LANDESMAN 9.1. Eigenvalues of unitary matrices 37 9.2. Application 39 9.3. Strong Szego limit theorem 40 10. 10/14/16 41 10.1. Background on Tableau 43 10.2. KOSKA Numbers 44 11. 10/17/16 45 11.1. Relations of skew-Schur functions to other fields 45 11.2. Characters of the symmetric group 46 12. 10/19/16 49 13. 10/21/16 55 13.1. -
21 Schur Indicator
21 Schur indicator Complex representation theory gives a good description of the homomorphisms from a group to a special unitary group. The Schur indicator describes when these are orthogonal or quaternionic, so it is also easy to describe all homomor- phisms to the compact orthogonal and symplectic groups (and a little bit of fiddling around with central extensions gives the homomorphisms to compact spin groups). So the homomorphisms to any compact classical group are well understood. However there seems to be no easy way to describe the homomor- phisms of a group to the exceptional compact Lie groups. We have several closely related problems: • Which irreducible representations have symmetric or alternating forms? • Classify the homomorphisms to orthogonal and symplectic groups • Classify the real and quaternionic representations given the complex ones. Suppose we have an irreducible representation V of a compact group G. We study the space of invariant bilinear forms on V . Obviously the bilinear forms correspond to maps from V to its dual, so the space of such forms is at most 1-dimensional, and is non-zero if and only if V is isomorphic to its dual, in other words if and only if the character of V is real. We also want to know when the bilinear form is symmetric or alternating. These two possibilities correspond to the symmetric or alternating square containing the 1-dimensional irreducible representation. So (1, χS2V − χΛ2V ) is 1, 0, or −1 depending on whether V has a symmetric bilinear form, no bilinear form, or an alternating bilinear form. By 2 the formulas for the symmetric and alternating squares this is given by G χg , and is called the Schur indicator. -
Master Thesis Written at the Max Planck Institute of Quantum Optics
Ludwig-Maximilians-Universitat¨ Munchen¨ and Technische Universitat¨ Munchen¨ A time-dependent Gaussian variational description of Lattice Gauge Theories Master thesis written at the Max Planck Institute of Quantum Optics September 2017 Pablo Sala de Torres-Solanot Ludwig-Maximilians-Universitat¨ Munchen¨ Technische Universitat¨ Munchen¨ Max-Planck-Institut fur¨ Quantenoptik A time-dependent Gaussian variational description of Lattice Gauge Theories First reviewer: Prof. Dr. Ignacio Cirac Second reviewer: Dr. Tao Shi Thesis submitted in partial fulfillment of the requirements for the degree of Master of Science within the programme Theoretical and Mathematical Physics Munich, September 2017 Pablo Sala de Torres-Solanot Abstract In this thesis we pursue the novel idea of using Gaussian states for high energy physics and explore some of the first necessary steps towards such a direction, via a time- dependent variational method. While these states have often been applied to con- densed matter systems via Hartree-Fock, BCS or generalized Hartree-Fock theory, this is not the case in high energy physics. Their advantage is the fact that they are completely characterized, via Wick's theorem, by their two-point correlation func- tions (and one-point averages in bosonic systems as well), e.g., all possible pairings between fermionic operators. These are collected in the so-called covariance matrix which then becomes the most relevant object in their description. In order to reach this goal, we set the theory on a lattice by making use of Lat- tice Gauge Theories (LGT). This method, introduced by Kenneth Wilson, has been extensively used for the study of gauge theories in non-perturbative regimes since it allows new analytical methods as for example strong coupling expansions, as well as the use of Monte Carlo simulations and more recently, Tensor Networks techniques as well. -
20 Representation Theory
20 Representation theory A representation of a group is an action of a group on something, in other words a homomorphism from the group to the group of automorphisms of something. The most obvious representations are permutation representations: actions of a group on a (discrete) set. For example the group of rotations of a cube has order 24, and has several obvious permutation representations: it can act on faces, edges, vertices, diagonals, pairs of opposite faces, and so on. For another example, the group SL2(R) acts on the real projective line, and on the upper half plane. These sets carry topologies, which we should take into account when defining representations. Let us try to classify all permutation representations of some group G . First of all, if the group G acts on some set X, then we can write X as the disjoint union of the orbits of G on X, and G is transitive on each of these orbits. So this reduces the classification of all permutation representations to that of transitive permutation representations. Next, given a transitive permutation representation of G on a set X, fix a point x ∈ X and write Gx for the subgroup fixing x. Then as a permutation representation, X is isomorphic to the action of G on the set of cosets G/Gx. If we choose a different point y, then Gx is conjugate to Gy (using some element of G taking x to y), so we see that transitive permutation representations up to isomorphism correspond to conjugacy classes of subgroups of G.