When Is the Numerical Range of a Nilpotent Matrix Circular?
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MATH 2370, Practice Problems
MATH 2370, Practice Problems Kiumars Kaveh Problem: Prove that an n × n complex matrix A is diagonalizable if and only if there is a basis consisting of eigenvectors of A. Problem: Let A : V ! W be a one-to-one linear map between two finite dimensional vector spaces V and W . Show that the dual map A0 : W 0 ! V 0 is surjective. Problem: Determine if the curve 2 2 2 f(x; y) 2 R j x + y + xy = 10g is an ellipse or hyperbola or union of two lines. Problem: Show that if a nilpotent matrix is diagonalizable then it is the zero matrix. Problem: Let P be a permutation matrix. Show that P is diagonalizable. Show that if λ is an eigenvalue of P then for some integer m > 0 we have λm = 1 (i.e. λ is an m-th root of unity). Hint: Note that P m = I for some integer m > 0. Problem: Show that if λ is an eigenvector of an orthogonal matrix A then jλj = 1. n Problem: Take a vector v 2 R and let H be the hyperplane orthogonal n n to v. Let R : R ! R be the reflection with respect to a hyperplane H. Prove that R is a diagonalizable linear map. Problem: Prove that if λ1; λ2 are distinct eigenvalues of a complex matrix A then the intersection of the generalized eigenspaces Eλ1 and Eλ2 is zero (this is part of the Spectral Theorem). 1 Problem: Let H = (hij) be a 2 × 2 Hermitian matrix. Use the Min- imax Principle to show that if λ1 ≤ λ2 are the eigenvalues of H then λ1 ≤ h11 ≤ λ2. -
Nilpotent Elements Control the Structure of a Module
Nilpotent elements control the structure of a module David Ssevviiri Department of Mathematics Makerere University, P.O BOX 7062, Kampala Uganda E-mail: [email protected], [email protected] Abstract A relationship between nilpotency and primeness in a module is investigated. Reduced modules are expressed as sums of prime modules. It is shown that presence of nilpotent module elements inhibits a module from possessing good structural properties. A general form is given of an example used in literature to distinguish: 1) completely prime modules from prime modules, 2) classical prime modules from classical completely prime modules, and 3) a module which satisfies the complete radical formula from one which is neither 2-primal nor satisfies the radical formula. Keywords: Semisimple module; Reduced module; Nil module; K¨othe conjecture; Com- pletely prime module; Prime module; and Reduced ring. MSC 2010 Mathematics Subject Classification: 16D70, 16D60, 16S90 1 Introduction Primeness and nilpotency are closely related and well studied notions for rings. We give instances that highlight this relationship. In a commutative ring, the set of all nilpotent elements coincides with the intersection of all its prime ideals - henceforth called the prime radical. A popular class of rings, called 2-primal rings (first defined in [8] and later studied in [23, 26, 27, 28] among others), is defined by requiring that in a not necessarily commutative ring, the set of all nilpotent elements coincides with the prime radical. In an arbitrary ring, Levitzki showed that the set of all strongly nilpotent elements coincides arXiv:1812.04320v1 [math.RA] 11 Dec 2018 with the intersection of all prime ideals, [29, Theorem 2.6]. -
Classifying the Representation Type of Infinitesimal Blocks of Category
Classifying the Representation Type of Infinitesimal Blocks of Category OS by Kenyon J. Platt (Under the Direction of Brian D. Boe) Abstract Let g be a simple Lie algebra over the field C of complex numbers, with root system Φ relative to a fixed maximal toral subalgebra h. Let S be a subset of the simple roots ∆ of Φ, which determines a standard parabolic subalgebra of g. Fix an integral weight ∗ µ µ ∈ h , with singular set J ⊆ ∆. We determine when an infinitesimal block O(g,S,J) := OS of parabolic category OS is nonzero using the theory of nilpotent orbits. We extend work of Futorny-Nakano-Pollack, Br¨ustle-K¨onig-Mazorchuk, and Boe-Nakano toward classifying the representation type of the nonzero infinitesimal blocks of category OS by considering arbitrary sets S and J, and observe a strong connection between the theory of nilpotent orbits and the representation type of the infinitesimal blocks. We classify certain infinitesimal blocks of category OS including all the semisimple infinitesimal blocks in type An, and all of the infinitesimal blocks for F4 and G2. Index words: Category O; Representation type; Verma modules Classifying the Representation Type of Infinitesimal Blocks of Category OS by Kenyon J. Platt B.A., Utah State University, 1999 M.S., Utah State University, 2001 M.A, The University of Georgia, 2006 A Thesis Submitted to the Graduate Faculty of The University of Georgia in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy Athens, Georgia 2008 c 2008 Kenyon J. Platt All Rights Reserved Classifying the Representation Type of Infinitesimal Blocks of Category OS by Kenyon J. -
Hyperbolicity of Hermitian Forms Over Biquaternion Algebras
HYPERBOLICITY OF HERMITIAN FORMS OVER BIQUATERNION ALGEBRAS NIKITA A. KARPENKO Abstract. We show that a non-hyperbolic hermitian form over a biquaternion algebra over a field of characteristic 6= 2 remains non-hyperbolic over a generic splitting field of the algebra. Contents 1. Introduction 1 2. Notation 2 3. Krull-Schmidt principle 3 4. Splitting off a motivic summand 5 5. Rost correspondences 7 6. Motivic decompositions of some isotropic varieties 12 7. Proof of Main Theorem 14 References 16 1. Introduction Throughout this note (besides of x3 and x4) F is a field of characteristic 6= 2. The basic reference for the staff related to involutions on central simple algebras is [12].p The degree deg A of a (finite dimensional) central simple F -algebra A is the integer dimF A; the index ind A of A is the degree of a central division algebra Brauer-equivalent to A. Conjecture 1.1. Let A be a central simple F -algebra endowed with an orthogonal invo- lution σ. If σ becomes hyperbolic over the function field of the Severi-Brauer variety of A, then σ is hyperbolic (over F ). In a stronger version of Conjecture 1.1, each of two words \hyperbolic" is replaced by \isotropic", cf. [10, Conjecture 5.2]. Here is the complete list of indices ind A and coindices coind A = deg A= ind A of A for which Conjecture 1.1 is known (over an arbitrary field of characteristic 6= 2), given in the chronological order: • ind A = 1 | trivial; Date: January 2008. Key words and phrases. -
Arxiv:1508.00183V2 [Math.RA] 6 Aug 2015 Atclrb Ed Yasemigroup a by field
A THEOREM OF KAPLANSKY REVISITED HEYDAR RADJAVI AND BAMDAD R. YAHAGHI Abstract. We present a new and simple proof of a theorem due to Kaplansky which unifies theorems of Kolchin and Levitzki on triangularizability of semigroups of matrices. We also give two different extensions of the theorem. As a consequence, we prove the counterpart of Kolchin’s Theorem for finite groups of unipotent matrices over division rings. We also show that the counterpart of Kolchin’s Theorem over division rings of characteristic zero implies that of Kaplansky’s Theorem over such division rings. 1. Introduction The purpose of this short note is three-fold. We give a simple proof of Kaplansky’s Theorem on the (simultaneous) triangularizability of semi- groups whose members all have singleton spectra. Our proof, although not independent of Kaplansky’s, avoids the deeper group theoretical aspects present in it and in other existing proofs we are aware of. Also, this proof can be adjusted to give an affirmative answer to Kolchin’s Problem for finite groups of unipotent matrices over division rings. In particular, it follows from this proof that the counterpart of Kolchin’s Theorem over division rings of characteristic zero implies that of Ka- plansky’s Theorem over such division rings. We also present extensions of Kaplansky’s Theorem in two different directions. M arXiv:1508.00183v2 [math.RA] 6 Aug 2015 Let us fix some notation. Let ∆ be a division ring and n(∆) the algebra of all n × n matrices over ∆. The division ring ∆ could in particular be a field. By a semigroup S ⊆ Mn(∆), we mean a set of matrices closed under multiplication. -
Chapter 6 Jordan Canonical Form
Chapter 6 Jordan Canonical Form 175 6.1 Primary Decomposition Theorem For a general matrix, we shall now try to obtain the analogues of the ideas we have in the case of diagonalizable matrices. Diagonalizable Case General Case Minimal Polynomial: Minimal Polynomial: k k Y rj Y rj mA(λ) = (λ − λj) mA(λ) = (λ − λj) j=1 j=1 where rj = 1 for all j where 1 ≤ rj ≤ aj for all j Eigenspaces: Eigenspaces: Wj = Null Space of (A − λjI) Wj = Null Space of (A − λjI) dim(Wj) = gj and gj = aj for all j dim(Wj) = gj and gj ≤ aj for all j Generalized Eigenspaces: rj Vj = Null Space of (A − λjI) dim(Vj) = aj Decomposition: Decomposition: n n F = W1 ⊕ W2 ⊕ Wj ⊕ · · · ⊕ Wk W = W1⊕W2⊕Wj⊕· · ·⊕Wk is a subspace of F Primary Decomposition Theorem: n F = V1 ⊕ V2 ⊕ Vj ⊕ Vk n n x 2 F =) 9 unique x 2 F =) 9 unique xj 2 Wj, 1 ≤ j ≤ k such that vj 2 Vj, 1 ≤ j ≤ k such that x = x1 + x2 + ··· + xj + ··· + xk x = v1 + v2 + ··· + vj + ··· + vk 176 6.2 Analogues of Lagrange Polynomial Diagonalizable Case General Case Define Define k k Y Y ri fj(λ) = (λ − λi) Fj(λ) = (λ − λi) i=1 i=1 i6=j i6=j This is a set of coprime polynomials This is a set of coprime polynomials and and hence there exist polynomials hence there exist polynomials Gj(λ), 1 ≤ gj(λ), 1 ≤ j ≤ k such that j ≤ k such that k k X X fj(λ)gj(λ) = 1 Fj(λ)Gj(λ) = 1 j=1 j=1 The polynomials The polynomials `j(λ) = fj(λ)gj(λ); 1 ≤ j ≤ k Lj(λ) = Fj(λ)Gj(λ); 1 ≤ j ≤ k are the Lagrange Interpolation are the counterparts of the polynomials Lagrange Interpolation polynomials `1(λ) + `2(λ) + ··· + `k(λ) = 1 L1(λ) + L2(λ) + ··· + Lk(λ) = 1 λ1`1(λ)+λ2`2(λ)+···+λk`k(λ) = λ λ1L1(λ) + λ2L2(λ) + ··· + λkLk(λ) = d(λ) (a polynomial but it need not be = λ) For i 6= j the product `i(λ)`j(λ) has For i 6= j the product Li(λ)Lj(λ) has a a factor mA (λ) factor mA (λ) 6.3 Matrix Decomposition In the diagonalizable case, using the Lagrange polynomials we obtained a decomposition of the matrix A. -
Commutative Algebra
Commutative Algebra Andrew Kobin Spring 2016 / 2019 Contents Contents Contents 1 Preliminaries 1 1.1 Radicals . .1 1.2 Nakayama's Lemma and Consequences . .4 1.3 Localization . .5 1.4 Transcendence Degree . 10 2 Integral Dependence 14 2.1 Integral Extensions of Rings . 14 2.2 Integrality and Field Extensions . 18 2.3 Integrality, Ideals and Localization . 21 2.4 Normalization . 28 2.5 Valuation Rings . 32 2.6 Dimension and Transcendence Degree . 33 3 Noetherian and Artinian Rings 37 3.1 Ascending and Descending Chains . 37 3.2 Composition Series . 40 3.3 Noetherian Rings . 42 3.4 Primary Decomposition . 46 3.5 Artinian Rings . 53 3.6 Associated Primes . 56 4 Discrete Valuations and Dedekind Domains 60 4.1 Discrete Valuation Rings . 60 4.2 Dedekind Domains . 64 4.3 Fractional and Invertible Ideals . 65 4.4 The Class Group . 70 4.5 Dedekind Domains in Extensions . 72 5 Completion and Filtration 76 5.1 Topological Abelian Groups and Completion . 76 5.2 Inverse Limits . 78 5.3 Topological Rings and Module Filtrations . 82 5.4 Graded Rings and Modules . 84 6 Dimension Theory 89 6.1 Hilbert Functions . 89 6.2 Local Noetherian Rings . 94 6.3 Complete Local Rings . 98 7 Singularities 106 7.1 Derived Functors . 106 7.2 Regular Sequences and the Koszul Complex . 109 7.3 Projective Dimension . 114 i Contents Contents 7.4 Depth and Cohen-Macauley Rings . 118 7.5 Gorenstein Rings . 127 8 Algebraic Geometry 133 8.1 Affine Algebraic Varieties . 133 8.2 Morphisms of Affine Varieties . 142 8.3 Sheaves of Functions . -
Nilpotent Ideals in Polynomial and Power Series Rings 1609
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 138, Number 5, May 2010, Pages 1607–1619 S 0002-9939(10)10252-4 Article electronically published on January 13, 2010 NILPOTENT IDEALS IN POLYNOMIAL AND POWER SERIES RINGS VICTOR CAMILLO, CHAN YONG HONG, NAM KYUN KIM, YANG LEE, AND PACE P. NIELSEN (Communicated by Birge Huisgen-Zimmermann) Abstract. Given a ring R and polynomials f(x),g(x) ∈ R[x] satisfying f(x)Rg(x) = 0, we prove that the ideal generated by products of the coef- ficients of f(x)andg(x) is nilpotent. This result is generalized, and many well known facts, along with new ones, concerning nilpotent polynomials and power series are obtained. We also classify which of the standard nilpotence properties on ideals pass to polynomial rings or from ideals in polynomial rings to ideals of coefficients in base rings. In particular, we prove that if I ≤ R[x]is aleftT -nilpotent ideal, then the ideal formed by the coefficients of polynomials in I is also left T -nilpotent. 1. Introduction Throughout this paper, all rings are associative rings with 1. It is well known that a polynomial f(x) over a commutative ring is nilpotent if and only if each coefficient of f(x) is nilpotent. But this result is not true in general for noncommutative rings. For example, let R = Mn(k), the n × n full matrix ring over some ring k =0. 2 Consider the polynomial f(x)=e12 +(e11 − e22)x − e21x ,wheretheeij’s are 2 the matrix units. In this case f(x) = 0, but e11 − e22 is not nilpotent. -
An Effective Lie–Kolchin Theorem for Quasi-Unipotent Matrices
Linear Algebra and its Applications 581 (2019) 304–323 Contents lists available at ScienceDirect Linear Algebra and its Applications www.elsevier.com/locate/laa An effective Lie–Kolchin Theorem for quasi-unipotent matrices Thomas Koberda a, Feng Luo b,∗, Hongbin Sun b a Department of Mathematics, University of Virginia, Charlottesville, VA 22904-4137, USA b Department of Mathematics, Rutgers University, Hill Center – Busch Campus, 110 Frelinghuysen Road, Piscataway, NJ 08854, USA a r t i c l e i n f oa b s t r a c t Article history: We establish an effective version of the classical Lie–Kolchin Received 27 April 2019 Theorem. Namely, let A, B ∈ GLm(C)be quasi-unipotent Accepted 17 July 2019 matrices such that the Jordan Canonical Form of B consists Available online 23 July 2019 of a single block, and suppose that for all k 0the Submitted by V.V. Sergeichuk matrix ABk is also quasi-unipotent. Then A and B have a A, B < C MSC: common eigenvector. In particular, GLm( )is a primary 20H20, 20F38 solvable subgroup. We give applications of this result to the secondary 20F16, 15A15 representation theory of mapping class groups of orientable surfaces. Keywords: © 2019 Elsevier Inc. All rights reserved. Lie–Kolchin theorem Unipotent matrices Solvable groups Mapping class groups * Corresponding author. E-mail addresses: [email protected] (T. Koberda), fl[email protected] (F. Luo), [email protected] (H. Sun). URLs: http://faculty.virginia.edu/Koberda/ (T. Koberda), http://sites.math.rutgers.edu/~fluo/ (F. Luo), http://sites.math.rutgers.edu/~hs735/ (H. -
Problem 1. an Element a of a Ring R Is Called Nilpotent If a M = 0 for Some M > 0. A) Prove That in a Commutative Ring R
Problem 1. An element a of a ring R is called nilpotent if am = 0 for some m> 0. a) Prove that in a commutative ring R the set N of all nilpotent elements of R is an ideal. This ideal is called the nilradical of R. Prove that 0 is the only nilpotent element of R/N. b) Let R be a commutative ring and let a1, ..., an R be nilpotent. Set I for the ∈ ideal < a1, ..., an > generated by a1, ..., an. Prove that there is a positive integer N N such that x1x2...xN = 0 for any x1, ..., xN in I (i.e. that I = 0). c) Prove that the set of all nilpotent elements in the ring M2(R) is not an ideal. d) Prove that if p is a prime and m > 0 then every element of Z/pmZ is either nilpotent or invertible. e) Find the nilradical of Z/36Z (by correspondence theorem, it is equal to nZ/36Z for some n). Solution:a) Suppose that a, b N and r R. Thus an = 0 and bm = 0 for ∈ ∈ some positive integers m, n. By the Newton’s binomial formula we have m+n m + n (a b)m+n = ai( b)m+n−i. (1) − i − i=0 X Note that, for every i 1, 2, ..., m+n , either i n or m+n i m and therefore ∈{ } ≥ − ≥ either ai =0or( b)m+n−i = 0. It follows that every summand in the sum (1) is 0, − so (a b)m+n = 0. Thus a b N. -
Semisimple Cyclic Elements in Semisimple Lie Algebras
Semisimple cyclic elements in semisimple Lie algebras A. G. Elashvili1 , M. Jibladze1 , and V. G. Kac2 1 Razmadze Mathematical Institute, TSU, Tbilisi 0186, Georgia 2 Department of Mathematics, MIT, Cambridge MA 02139, USA Abstract This paper is a continuation of the theory of cyclic elements in semisimple Lie algebras, developed by Elashvili, Kac and Vinberg. Its main result is the classification of semisimple cyclic elements in semisimple Lie algebras. The importance of this classification stems from the fact that each such element gives rise to an integrable hierarchy of Hamiltonian PDE of Drinfeld-Sokolov type. 1 Introduction Let g be a semisimple finite-dimensional Lie algebra over an algebraically closed field F of characteristic 0 and let e be a non-zero nilpotent element of g. By the Morozov- Jacobson theorem, the element e can be included in an sl(2)-triple s = fe; h; fg (unique, up to conjugacy [Ko]), so that [e; f] = h,[h; e] = 2e,[h; f] = −2f. Then the eigenspace decomposition of g with respect to ad h is a Z-grading of g: d M (1.1) g = gj; where g±d 6= 0. j=−d The positive integer d is called the depth of the nilpotent element e. An element of g of the form e + F , where F is a non-zero element of g−d, is called a cyclic element, associated to e. In [Ko] Kostant proved that any cyclic element, associated to a principal (= regular) nilpotent element e, is regular semisimple, and in [Sp] Springer proved that any cyclic element, associated to a subregular nilpotent element of a simple exceptional Lie algebra, is regular semisimple as well, and, moreover, found two more distinguished nilpotent elements in E8 with the same property. -
Are Octonions Necessary to the Standard Model?
Vigier IOP Publishing IOP Conf. Series: Journal of Physics: Conf. Series 1251 (2019) 012044 doi:10.1088/1742-6596/1251/1/012044 Are octonions necessary to the Standard Model? Peter Rowlands, Sydney Rowlands Physics Department, University of Liverpool, Oliver Lodge Laboratory, Oxford St, Liverpool. L69 7ZE, UK [email protected] Abstract. There have been a number of claims, going back to the 1970s, that the Standard Model of particle physics, based on fermions and antifermions, might be derived from an octonion algebra. The emergence of SU(3), SU(2) and U(1) groups in octonion-based structures is suggestive of the symmetries of the Standard Model, but octonions themselves are an unsatisfactory model for physical application because they are antiassociative and consequently not a group. Instead, the ‘octonion’ models have to be based on adjoint algebras, such as left- or right-multiplied octonions, which can be seen to have group-like properties. The most promising of these candidates is the complexified left-multiplied octonion algebra, because it reduces, in effect, to Cl(6), which has been identified by one of us (PR) in a number of previous publications as the basic structure for the entire foundation of physics, as well as the algebra required for the Standard Model and the Dirac equation. Though this algebra has long been shown by PR as equivalent to using a complexified left-multiplied or ‘broken’ octonion, it doesn’t need to be derived in this way, as its real origins are in the respective real, complex, quaternion and complexified quaternion algebras of the fundamental parameters of mass, time, charge and space.