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Multiplicative Theory of Ideals This Is Volume 43 in PURE and APPLIED MATHEMATICS a Series of Monographs and Textbooks Editors: PAULA
Multiplicative Theory of Ideals This is Volume 43 in PURE AND APPLIED MATHEMATICS A Series of Monographs and Textbooks Editors: PAULA. SMITHAND SAMUELEILENBERG A complete list of titles in this series appears at the end of this volume MULTIPLICATIVE THEORY OF IDEALS MAX D. LARSEN / PAUL J. McCARTHY University of Nebraska University of Kansas Lincoln, Nebraska Lawrence, Kansas @ A CADEM I C P RE S S New York and London 1971 COPYRIGHT 0 1971, BY ACADEMICPRESS, INC. ALL RIGHTS RESERVED NO PART OF THIS BOOK MAY BE REPRODUCED IN ANY FORM, BY PHOTOSTAT, MICROFILM, RETRIEVAL SYSTEM, OR ANY OTHER MEANS, WITHOUT WRITTEN PERMISSION FROM THE PUBLISHERS. ACADEMIC PRESS, INC. 111 Fifth Avenue, New York, New York 10003 United Kingdom Edition published by ACADEMIC PRESS, INC. (LONDON) LTD. Berkeley Square House, London WlX 6BA LIBRARY OF CONGRESS CATALOG CARD NUMBER: 72-137621 AMS (MOS)1970 Subject Classification 13F05; 13A05,13B20, 13C15,13E05,13F20 PRINTED IN THE UNITED STATES OF AMERICA To Lillie and Jean This Page Intentionally Left Blank Contents Preface xi ... Prerequisites Xlll Chapter I. Modules 1 Rings and Modules 1 2 Chain Conditions 8 3 Direct Sums 12 4 Tensor Products 15 5 Flat Modules 21 Exercises 27 Chapter II. Primary Decompositions and Noetherian Rings 1 Operations on Ideals and Submodules 36 2 Primary Submodules 39 3 Noetherian Rings 44 4 Uniqueness Results for Primary Decompositions 48 Exercises 52 Chapter Ill. Rings and Modules of Quotients 1 Definition 61 2 Extension and Contraction of Ideals 66 3 Properties of Rings of Quotients 71 Exercises 74 Vii Vlll CONTENTS Chapter IV. -
3D Gauge Theories, Symplectic Duality and Knot Homology I
3d Gauge Theories, Symplectic Duality and Knot Homology I Tudor Dimofte Notes by Qiaochu Yuan December 8, 2014 We want to study some 3d N = 4 supersymmetric QFTs. They won't be topological, but the supersymmetry will still help. We'll look in particular at boundary conditions and compactifications to 2d. Most of this material is relatively old by physics standards (known since the '90s). A motivation for discussing these theories here is that they seem closely related to 1. geometric representation theory, 2. geometric constructions of knot homologies, and 3. symplectic duality. This story gives rise to some interesting mathematical predictions. On Tuesday we'll talk about what symplectic n-ality should mean. On Wednesday we'll give a new construction of projectives in variants of category O. On Thursday we'll talk about category O and knot homologies, and a new approach to both via 2d Landau-Ginzburg models. 1 Geometric representation theory For starters, let G = SL2. The universal enveloping algebra of its Lie algebra is U(sl2) = hE; F; H j [E; F ] = H; [H; E] = 2E; [H; F ] = −2F i: (1) The center is generated by the Casimir operator 1 χ = EF + FE + H2: (2) 2 The full category of U(sl2)-modules is hard to work with. Bernstein, Gelfand, and Gelfand proposed that we work in a nice subcategory O of highest weight representations (on which E acts locally finitely or locally nilpotently, depending on the definition) decomposing as a sum M M = Mµ (3) µ of generalized eigenspaces with respect to the action of the generator of the Cartan L subalgebra H. -
Open Problems
Open Problems 1. Does the lower radical construction for `-rings stop at the first infinite ordinal (Theorems 3.2.5 and 3.2.8)? This is the case for rings; see [ADS]. 2. If P is a radical class of `-rings and A is an `-ideal of R, is P(A) an `-ideal of R (Theorem 3.2.16 and Exercises 3.2.24 and 3.2.25)? 3. (Diem [DI]) Is an sp-`-prime `-ring an `-domain (Theorem 3.7.3)? 4. If R is a torsion-free `-prime `-algebra over the totally ordered domain C and p(x) 2C[x]nC with p0(1) > 0 in C and p(a) ¸ 0 for every a 2 R, is R an `-domain (Theorems 3.8.3 and 3.8.4)? 5. Does each f -algebra over a commutative directed po-unital po-ring C whose left and right annihilator ideals vanish have a unique tight C-unital cover (Theorems 3.4.5, 3.4.11, and 3.4.12 and Exercises 3.4.16 and 3.4.18)? 6. Can an f -ring contain a principal `-idempotent `-ideal that is not generated by an upperpotent element (Theorem 3.4.4 and Exercise 3.4.15)? 7. Is each C-unital cover of a C-unitable (totally ordered) f -algebra (totally or- dered) tight (Theorem 3.4.10)? 8. Is an archimedean `-group a nonsingular module over its f -ring of f -endomorphisms (Exercise 4.3.56)? 9. If an archimedean `-group is a finitely generated module over its ring of f -endomorphisms, is it a cyclic module (Exercise 3.6.20)? 10. -
Parabolic Category O for Classical Lie Superalgebras
Parabolic category O for classical Lie superalgebras Volodymyr Mazorchuk Abstract We compare properties of (the parabolic version of) the BGG category O for semi-simple Lie algebras with those for classical (not necessarily simple) Lie superalgebras. 1 Introduction Category O for semi-simple complex finite dimensional Lie algebras, introduced in [BGG], is a central object of study in the modern representation theory (see [Hu]) with many interesting connections to, in particular, combinatorics, alge- braic geometry and topology. This category has a natural counterpart in the super- world and this super version O˜ of category O was intensively studied (mostly for some particular simple classical Lie superalgebra) in the last decade, see e.g. [Br1, Br2, Go2, FM2, CLW, CMW] or the recent books [Mu, CW] for details. The aim of the present paper is to compare some basic but general properties of the category O in the non-super and super cases for a rather general classical super-setup. We mainly restrict to the properties for which the non-super and super cases can be connected using the usual restriction and induction functors and the biadjunction (up to parity change) between these two functors is our main tool. The paper also complements, extends and gives a more detailed exposition for some results which appeared in [AM, Section 7]. The original category O has a natural parabolic version which first appeared in [RC]. We start in Section 2 by setting up an elementary approach (using root system geometry) to the definition of a parabolic category O for classical finite dimensional Lie superalgebras. -
Geometric Representation Theory, Fall 2005
GEOMETRIC REPRESENTATION THEORY, FALL 2005 Some references 1) J. -P. Serre, Complex semi-simple Lie algebras. 2) T. Springer, Linear algebraic groups. 3) A course on D-modules by J. Bernstein, availiable at www.math.uchicago.edu/∼arinkin/langlands. 4) J. Dixmier, Enveloping algebras. 1. Basics of the category O 1.1. Refresher on semi-simple Lie algebras. In this course we will work with an alge- braically closed ground field of characteristic 0, which may as well be assumed equal to C Let g be a semi-simple Lie algebra. We will fix a Borel subalgebra b ⊂ g (also sometimes denoted b+) and an opposite Borel subalgebra b−. The intersection b+ ∩ b− is a Cartan subalgebra, denoted h. We will denote by n, and n− the unipotent radicals of b and b−, respectively. We have n = [b, b], and h ' b/n. (I.e., h is better to think of as a quotient of b, rather than a subalgebra.) The eigenvalues of h acting on n are by definition the positive roots of g; this set will be denoted by ∆+. We will denote by Q+ the sub-semigroup of h∗ equal to the positive span of ∆+ (i.e., Q+ is the set of eigenvalues of h under the adjoint action on U(n)). For λ, µ ∈ h∗ we shall say that λ ≥ µ if λ − µ ∈ Q+. We denote by P + the sub-semigroup of dominant integral weights, i.e., those λ that satisfy hλ, αˇi ∈ Z+ for all α ∈ ∆+. + For α ∈ ∆ , we will denote by nα the corresponding eigen-space. -
Arxiv:1907.06685V1 [Math.RT]
CATEGORY O FOR TAKIFF sl2 VOLODYMYR MAZORCHUK AND CHRISTOFFER SODERBERG¨ Abstract. We investigate various ways to define an analogue of BGG category O for the non-semi-simple Takiff extension of the Lie algebra sl2. We describe Gabriel quivers for blocks of these analogues of category O and prove extension fullness of one of them in the category of all modules. 1. Introduction and description of the results The celebrated BGG category O, introduced in [BGG], is originally associated to a triangular decomposition of a semi-simple finite dimensional complex Lie algebra. The definition of O is naturally generalized to all Lie algebras admitting some analogue of a triangular decomposition, see [MP]. These include, in particular, Kac-Moody algebras and Virasoro algebra. Category O has a number of spectacular properties and applications to various areas of mathematics, see for example [Hu] and references therein. The paper [DLMZ] took some first steps in trying to understand structure and prop- erties of an analogue of category O in the case of a non-reductive finite dimensional Lie algebra. The investigation in [DLMZ] focuses on category O for the so-called Schr¨odinger algebra, which is a central extension of the semi-direct product of sl2 with its natural 2-dimensional module. It turned out that, for the Schr¨odinger algebra, the behavior of blocks of category O with non-zero central charge is exactly the same as the behavior of blocks of category O for the algebra sl2. At the same, block with zero central charge turned out to be significantly more difficult. -
Algebraic Numbers
FORMALIZED MATHEMATICS Vol. 24, No. 4, Pages 291–299, 2016 DOI: 10.1515/forma-2016-0025 degruyter.com/view/j/forma Algebraic Numbers Yasushige Watase Suginami-ku Matsunoki 6 3-21 Tokyo, Japan Summary. This article provides definitions and examples upon an integral element of unital commutative rings. An algebraic number is also treated as consequence of a concept of “integral”. Definitions for an integral closure, an algebraic integer and a transcendental numbers [14], [1], [10] and [7] are included as well. As an application of an algebraic number, this article includes a formal proof of a ring extension of rational number field Q induced by substitution of an algebraic number to the polynomial ring of Q[x] turns to be a field. MSC: 11R04 13B21 03B35 Keywords: algebraic number; integral dependency MML identifier: ALGNUM 1, version: 8.1.05 5.39.1282 1. Preliminaries From now on i, j denote natural numbers and A, B denote rings. Now we state the propositions: (1) Let us consider rings L1, L2, L3. Suppose L1 is a subring of L2 and L2 is a subring of L3. Then L1 is a subring of L3. (2) FQ is a subfield of CF. (3) FQ is a subring of CF. R (4) Z is a subring of CF. Let us consider elements x, y of B and elements x1, y1 of A. Now we state the propositions: (5) If A is a subring of B and x = x1 and y = y1, then x + y = x1 + y1. (6) If A is a subring of B and x = x1 and y = y1, then x · y = x1 · y1. -
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. -
An Introduction to Affine Kac-Moody Algebras
An introduction to affine Kac-Moody algebras David Hernandez To cite this version: David Hernandez. An introduction to affine Kac-Moody algebras. DEA. Lecture notes from CTQM Master Class, Aarhus University, Denmark, October 2006, 2006. cel-00112530 HAL Id: cel-00112530 https://cel.archives-ouvertes.fr/cel-00112530 Submitted on 9 Nov 2006 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. AN INTRODUCTION TO AFFINE KAC-MOODY ALGEBRAS DAVID HERNANDEZ Abstract. In these lectures we give an introduction to affine Kac- Moody algebras, their representations, and applications of this the- ory. Contents 1. Introduction 1 2. Quick review on semi-simple Lie algebras 2 3. Affine Kac-Moody algebras 5 4. Representations of Lie algebras 8 5. Fusion product, conformal blocks and Knizhnik- Zamolodchikov equations 14 References 19 1. Introduction Affine Kac-Moody algebras ˆg are infinite dimensional analogs of semi-simple Lie algebras g and have a central role both in Mathematics (Modular forms, Geometric Langlands program...) and Mathematical Physics (Conformal Field Theory...). These lectures are an introduction to the theory of affine Kac-Moody algebras and their representations with basic results and constructions to enter the theory. -
7902127 Fordt DAVID JAKES Oni the COMPUTATION of THE
7902127 FORDt DAVID JAKES ON i THE COMPUTATION OF THE MAXIMAL ORDER IK A DEDEKIND DOMAIN. THE OHIO STATE UNIVERSITY, PH.D*, 1978 University. Microfilms International 3q o n . z e e b r o a o . a n n a r b o r , mi 48ios ON THE COMPUTATION OF THE MAXIMAL ORDER IN A DEDEKIND DOMAIN DISSERTATION Presented in Partial Fulfillment of the Requirements for the Degree Doctor of Philosophy in the Graduate School of The Ohio State University By David James Ford, B.S., M.S. # * * K * The Ohio State University 1978 Reading Committee: Approved By Paul Ponomarev Jerome Rothstein Hans Zassenhaus Hans Zassenhaus Department of Mathematics ACKNOWLDEGMENTS I must first acknowledge the help of my Adviser, Professor Hans Zassenhaus, who was a fountain of inspiration whenever I was dry. I must also acknowlegde the help, financial and otherwise, that my parents gave me. Without it I could not have finished this work. All of the computing in this project, amounting to between one and two thousand hours of computer time, was done on a PDP-11 belonging to Drake and Ford Engineers, through the generosity of my father. VITA October 28, 1946.......... Born - Columbus, Ohio 1967...................... B.S. in Mathematics Massachusetts Institute of Technology Cambridge, Massachusetts 1967-196 8 ................. Teaching Assistant Department of Mathematics The Ohio State University Columbus, Ohio 1968-197 1................. Programmer Children's Hospital Medical Center Boston, Massachusetts 1971-1975................. Teaching Associate Department of Mathematics The Ohio State University Columbus, Ohio 1975-1978................. Programmer Prindle and Patrick, Architects Columbus, Ohio PUBLICATIONS "Relations in Q (Zh X ZQ) and Q (ZD X ZD)" (with Michael Singer) n 4 o n o o Communications in Algebra, Vol. -
Norms and Traces MAT4250 — Høst 2013 Norms and Traces
Norms and traces MAT4250 — Høst 2013 Norms and traces Version 0.2 — 10. september 2013 klokken 09:55 We start by recalling a few facts from linear algebra that will be very useful for us, and we shall do it over a general base field K (of any characteristic). Assume that V is afinitedimensionalvectorspaceoverK.Toanylinearoperatorφ: V V there are ! associated two polynomials, both in a canonical way. Firstly, there is the characteristic polynomial Pφ(t), which is, as we know, defined by Pφ(t)=det(t id φ). It is a monic polynomial whose degree n equals the dimension · − dimK V .TwoofthecoefficientsofPφ(t) play a special prominent role, the trace and the determinant. They are up to sign, respectively the coefficient of the subdominant term and the constant term of the characteristic polynomial Pφ(t): n n 1 n P (t)=t tr φt − + +( 1) det φ φ − ··· − Secondly, there is the minimal polynomial of φ.Itisdefinedasthemonicgenerator of the annihilator of φ,thatisthemonicgeneratoroftheidealIφ = f(t) K[t] { 2 | f(φ)=0 . The two polynomials arise in very different ways, but they are intimately } related. The Cayley-Hamilton theorem states that Pφ(φ)=0,sothecharacteristic polynomial of φ belongs to the ideal Iφ,andtheminimalpolynomialdividesthecha- racteristic polynomial. In general they are different. For example, the degree of the characteristic poly is always equal to dimK V ,butthedegreeoftheminimalpolycan be anything between one and dimK V (degree one occurring for scalar multiples of the identity map). We often will work over extensions ⌦ of the base field K.AvectorspaceV and alinearoperatorφ may accordingly be extended as the tensor products V K ⌦ and ⌦ φ idK .Ifv1,...,vn is a basis for V ,thenv1 1,...,vn 1 will be a basis for V K ⌦— ⌦ ⌦ ⌦ ⌦ the only thing that changes, is that we are allowed to use elements from ⌦ as coefficients. -
Notes on Ring Theory
Notes on Ring Theory by Avinash Sathaye, Professor of Mathematics February 1, 2007 Contents 1 1 Ring axioms and definitions. Definition: Ring We define a ring to be a non empty set R together with two binary operations f,g : R × R ⇒ R such that: 1. R is an abelian group under the operation f. 2. The operation g is associative, i.e. g(g(x, y),z)=g(x, g(y,z)) for all x, y, z ∈ R. 3. The operation g is distributive over f. This means: g(f(x, y),z)=f(g(x, z),g(y,z)) and g(x, f(y,z)) = f(g(x, y),g(x, z)) for all x, y, z ∈ R. Further we define the following natural concepts. 1. Definition: Commutative ring. If the operation g is also commu- tative, then we say that R is a commutative ring. 2. Definition: Ring with identity. If the operation g has a two sided identity then we call it the identity of the ring. If it exists, the ring is said to have an identity. 3. The zero ring. A trivial example of a ring consists of a single element x with both operations trivial. Such a ring leads to pathologies in many of the concepts discussed below and it is prudent to assume that our ring is not such a singleton ring. It is called the “zero ring”, since the unique element is denoted by 0 as per convention below. Warning: We shall always assume that our ring under discussion is not a zero ring.