Embedding Orders in Central Simple Algebras
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The Class Number One Problem for Imaginary Quadratic Fields
MODULAR CURVES AND THE CLASS NUMBER ONE PROBLEM JEREMY BOOHER Gauss found 9 imaginary quadratic fields with class number one, and in the early 19th century conjectured he had found all of them. It turns out he was correct, but it took until the mid 20th century to prove this. Theorem 1. Let K be an imaginary quadratic field whose ring of integers has class number one. Then K is one of p p p p p p p p Q(i); Q( −2); Q( −3); Q( −7); Q( −11); Q( −19); Q( −43); Q( −67); Q( −163): There are several approaches. Heegner [9] gave a proof in 1952 using the theory of modular functions and complex multiplication. It was dismissed since there were gaps in Heegner's paper and the work of Weber [18] on which it was based. In 1967 Stark gave a correct proof [16], and then noticed that Heegner's proof was essentially correct and in fact equiv- alent to his own. Also in 1967, Baker gave a proof using lower bounds for linear forms in logarithms [1]. Later, Serre [14] gave a new approach based on modular curve, reducing the class number + one problem to finding special points on the modular curve Xns(n). For certain values of n, it is feasible to find all of these points. He remarks that when \N = 24 An elliptic curve is obtained. This is the level considered in effect by Heegner." Serre says nothing more, and later writers only repeat this comment. This essay will present Heegner's argument, as modernized in Cox [7], then explain Serre's strategy. -
MAXIMAL and NON-MAXIMAL ORDERS 1. Introduction Let K Be A
MAXIMAL AND NON-MAXIMAL ORDERS LUKE WOLCOTT Abstract. In this paper we compare and contrast various prop- erties of maximal and non-maximal orders in the ring of integers of a number field. 1. Introduction Let K be a number field, and let OK be its ring of integers. An order in K is a subring R ⊆ OK such that OK /R is finite as a quotient of abelian groups. From this definition, it’s clear that there is a unique maximal order, namely OK . There are many properties that all orders in K share, but there are also differences. The main difference between a non-maximal order and the maximal order is that OK is integrally closed, but every non-maximal order is not. The result is that many of the nice properties of Dedekind domains do not hold in arbitrary orders. First we describe properties common to both maximal and non-maximal orders. In doing so, some useful results and constructions given in class for OK are generalized to arbitrary orders. Then we de- scribe a few important differences between maximal and non-maximal orders, and give proofs or counterexamples. Several proofs covered in lecture or the text will not be reproduced here. Throughout, all rings are commutative with unity. 2. Common Properties Proposition 2.1. The ring of integers OK of a number field K is a Noetherian ring, a finitely generated Z-algebra, and a free abelian group of rank n = [K : Q]. Proof: In class we showed that OK is a free abelian group of rank n = [K : Q], and is a ring. -
Artinian Subrings of a Commutative Ring
transactions of the american mathematical society Volume 336, Number 1, March 1993 ARTINIANSUBRINGS OF A COMMUTATIVERING ROBERT GILMER AND WILLIAM HEINZER Abstract. Given a commutative ring R, we investigate the structure of the set of Artinian subrings of R . We also consider the family of zero-dimensional subrings of R. Necessary and sufficient conditions are given in order that every zero-dimensional subring of a ring be Artinian. We also consider closure properties of the set of Artinian subrings of a ring with respect to intersection or finite intersection, and the condition that the set of Artinian subrings of a ring forms a directed family. 1. Introduction Suppose R is a commutative ring with unity element. We consider here various properties of the family sf of Artinian subrings of R and the family Z of zero-dimensional subrings of R . We remark that the inclusion s? ç Z may be proper, even if R is Noetherian; for example, Corollary 3.4 implies that if K is an infinite field of positive characteristic, then the local principal ideal ring K[X]/(X2) contains a zero-dimensional subring that is not Artinian. Of course, if every subring of R were Noetherian, the families sf and Z would be identical. Thus one source of motivation for this work comes from papers such as [Gi, Wi, W2, GHi, GH3] that deal with Noetherian and zero- dimensional pairs of rings, hereditarily Noetherian rings, and hereditarily zero- dimensional rings. Another source of motivation is related to our work in [GH3], where we considered several problems concerning a direct product of zero-dimensional rings. -
Maximal Orders of Quaternions
Maximal Orders of Quaternions Alyson Deines Quaternion Algebras Maximal Orders of Quaternions Maximal Orders Norms, Traces, and Alyson Deines Integrality Local Fields and Hilbert Symbols December 8th Math 581b Final Project Uses A non-commutative analogue of Rings of Integers of Number Field Abstract Maximal Orders of Quaternions Alyson Deines Abstract Quaternion I will define maximal orders of quaternion algebras, give Algebras Maximal examples, discuss how they are similar to and differ from rings Orders of integers, and then I will discuss one of their applications . Norms, Traces, and Integrality Local Fields and Hilbert Symbols Uses Quaternion Algebras over Number Fields Maximal Orders of Definition Quaternions Alyson Deines Let F be a field and a; b 2 F . A quaternion algebra over F is an F -algebra B = a;b Quaternion F Algebras with basis Maximal 2 2 Orders i = a; j = b; and ij = −ji: Norms, Traces, and Integrality Examples: Local Fields −1;−1 and Hilbert = Symbols H R p Uses −1;−1 F = Q( 5), B = F 1;b ∼ Let F be any number field, F = M2(F ) via 1 0 0 b i 7! and j 7! 0 −1 1 0 Maximal Orders Maximal Orders of Quaternions Lattices Alyson Deines Let F be a number field with ring of integers R and let V Quaternion be a finite dimensional F -vector space. Algebras An R-lattice of V is a finitely generated R-submodule Maximal Orders O ⊂ V such that OF = V . Norms, Traces, and Integrality Orders Local Fields and Hilbert Let F be a number field with ring of integers R and let B Symbols be a finite dimensional F -algebra. -
Ring (Mathematics) 1 Ring (Mathematics)
Ring (mathematics) 1 Ring (mathematics) In mathematics, a ring is an algebraic structure consisting of a set together with two binary operations usually called addition and multiplication, where the set is an abelian group under addition (called the additive group of the ring) and a monoid under multiplication such that multiplication distributes over addition.a[›] In other words the ring axioms require that addition is commutative, addition and multiplication are associative, multiplication distributes over addition, each element in the set has an additive inverse, and there exists an additive identity. One of the most common examples of a ring is the set of integers endowed with its natural operations of addition and multiplication. Certain variations of the definition of a ring are sometimes employed, and these are outlined later in the article. Polynomials, represented here by curves, form a ring under addition The branch of mathematics that studies rings is known and multiplication. as ring theory. Ring theorists study properties common to both familiar mathematical structures such as integers and polynomials, and to the many less well-known mathematical structures that also satisfy the axioms of ring theory. The ubiquity of rings makes them a central organizing principle of contemporary mathematics.[1] Ring theory may be used to understand fundamental physical laws, such as those underlying special relativity and symmetry phenomena in molecular chemistry. The concept of a ring first arose from attempts to prove Fermat's last theorem, starting with Richard Dedekind in the 1880s. After contributions from other fields, mainly number theory, the ring notion was generalized and firmly established during the 1920s by Emmy Noether and Wolfgang Krull.[2] Modern ring theory—a very active mathematical discipline—studies rings in their own right. -
Algebraic Groups I. Homework 8 1. Let a Be a Central Simple Algebra Over a field K, T a K-Torus in A×
Algebraic Groups I. Homework 8 1. Let A be a central simple algebra over a field k, T a k-torus in A×. (i) Adapt Exercise 5 in HW5 to make an ´etalecommutative k-subalgebra AT ⊆ A such that (AT )ks is × generated by T (ks), and establish a bijection between the sets of maximal k-tori in A and maximal ´etale commutative k-subalgebras of A. Deduce that SL(A) is k-anisotropic if and only if A is a division algebra. (ii) For an ´etalecommutative k-subalgebra C ⊆ A, prove ZA(C) is a semisimple k-algebra with center C. × (iv) If T is maximal as a k-split subtorus of A prove T is the k-group of units in AT and that the (central!) simple factors Bi of BT := ZA(AT ) are division algebras. (v) Fix A ' EndD(V ) for a right module V over a central division algebra D, so V is a left A-module and Q × V = Vi with nonzero left Bi-modules Vi. If T is maximal as a k-split torus in A , prove Vi has rank 1 × × over Bi and D, so Bi ' D. Using D-bases, deduce that all maximal k-split tori in A are A (k)-conjugate. 2. For a torus T over a local field k (allow R, C), prove T is k-anisotropic if and only if T (k) is compact. 3. Let Y be a smooth separated k-scheme locally of finite type, and T a k-torus with a left action on Y . -
Subfields of Central Simple Algebras
The Brauer Group Subfields of Algebras Subfields of Central Simple Algebras Patrick K. McFaddin University of Georgia Feb. 24, 2016 Patrick K. McFaddin University of Georgia Subfields of Central Simple Algebras The Brauer Group Subfields of Algebras Introduction Central simple algebras and the Brauer group have been well studied over the past century and have seen applications to class field theory, algebraic geometry, and physics. Since higher K-theory defined in '72, the theory of algebraic cycles have been utilized to study geometric objects associated to central simple algebras (with involution). This new machinery has provided a functorial viewpoint in which to study questions of arithmetic. Patrick K. McFaddin University of Georgia Subfields of Central Simple Algebras The Brauer Group Subfields of Algebras Central Simple Algebras Let F be a field. An F -algebra A is a ring with identity 1 such that A is an F -vector space and α(ab) = (αa)b = a(αb) for all α 2 F and a; b 2 A. The center of an algebra A is Z(A) = fa 2 A j ab = ba for every b 2 Ag: Definition A central simple algebra over F is an F -algebra whose only two-sided ideals are (0) and (1) and whose center is precisely F . Examples An F -central division algebra, i.e., an algebra in which every element has a multiplicative inverse. A matrix algebra Mn(F ) Patrick K. McFaddin University of Georgia Subfields of Central Simple Algebras The Brauer Group Subfields of Algebras Why Central Simple Algebras? Central simple algebras are a natural generalization of matrix algebras. -
A Brief History of Ring Theory
A Brief History of Ring Theory by Kristen Pollock Abstract Algebra II, Math 442 Loyola College, Spring 2005 A Brief History of Ring Theory Kristen Pollock 2 1. Introduction In order to fully define and examine an abstract ring, this essay will follow a procedure that is unlike a typical algebra textbook. That is, rather than initially offering just definitions, relevant examples will first be supplied so that the origins of a ring and its components can be better understood. Of course, this is the path that history has taken so what better way to proceed? First, it is important to understand that the abstract ring concept emerged from not one, but two theories: commutative ring theory and noncommutative ring the- ory. These two theories originated in different problems, were developed by different people and flourished in different directions. Still, these theories have much in com- mon and together form the foundation of today's ring theory. Specifically, modern commutative ring theory has its roots in problems of algebraic number theory and algebraic geometry. On the other hand, noncommutative ring theory originated from an attempt to expand the complex numbers to a variety of hypercomplex number systems. 2. Noncommutative Rings We will begin with noncommutative ring theory and its main originating ex- ample: the quaternions. According to Israel Kleiner's article \The Genesis of the Abstract Ring Concept," [2]. these numbers, created by Hamilton in 1843, are of the form a + bi + cj + dk (a; b; c; d 2 R) where addition is through its components 2 2 2 and multiplication is subject to the relations i =pj = k = ijk = −1. -
Differential Central Simple Algebras and Picard–Vessiot
Differential Central Simple Algebras and Picard–Vessiot Representations Lourdes Juan Department of Mathematics Texas Tech University Lubbock TX 79409 Andy R. Magid Department of Mathematics University of Oklahoma Norman OK 73019 March 7, 2007 Abstract A differential central simple algebra, and in particular a differential matrix algebra, over a differential field K with constants C can be trivial- ized by a Picard–Vessiot (differential Galois) extension E. In the matrix algebra case, there is a correspondence between K algebras trivialized by E and representations of the Galois group of E over K in P GLn(C), which can be interpreted as cocyles equivalent up to coboundaries. 1 Introduction Let K be a differential field with algebraically closed characteristic zero field of constants C and derivation D = DK . By a differential central simple al- gebra (DCSA) over K we mean a pair (A, D) where A is a central simple K algebra and D is a derivation of A extending the derivation D of its center K. Given two such pairs (A1, D1) and (A2, D2), we can form the differential algebra (A1 ⊗ A2, D1 ⊗ D2), where the derivation D1 ⊗ D2 is given by D1 ⊗ 1 + 1 ⊗ D2. Morphisms of DCSA’s over K are K algebra homomorphisms preserving deriva- tions. We denote the isomorphism class of (A, D) by [A, D]. The above tensor product defines a monoid operation on the isomorphism classes (the identity being the class [K, DK ]), and hence we can form the corresponding universal diff group K0 Az(K). (A central simple algebra (CSA) over a field is a special case of Azumaya, or central separable, algebras over rings; Az is an abbre- viation for Azumaya.) The corresponding object for K when derivations are not considered is the familiar K0Az(K) as defined by Bass in [1, Chapter III]. -
Lecture 2 Central Simple Algebras Patricio Quiroz
Lecture 2 Central Simple Algebras Patricio Quiroz Wesleyan University 04.08.2014 Remember that the theory of spinor genera is the \abelian part" in the problem of study the difference between local and global information, that is: gen(Λ) = GA:Λ j 0 spn(Λ) = GGA:Λ jj If G is not compact at some archimedean place. cls(Λ) = G:Λ where ∗ #fspinor genera in gen(Λ)g = jJK =K HA(Λ)j = [ΣΛ : K]; 1 n and HA(Λ) is the \image" of the spinor norm ΘA : GA ! JK =JK . This theory can be used to study representation problems as: Given a lattice M ⊂ Λ (Λ fixed of maximal rank), how many classes (orbits G:Λ) in the genus of Λ (in the orbit GA:Λ) contain an isomorphic copy of M? We will focus on the case of orders (lattices with additional structure) in central simple algebras (CSA's). So, we have to have some background material about CSA's and orders inside them. Motivation. Central simple algebras and orders appear in different places, for instance: 1. Number theory. Brauer groups play a central role in class field theory. 2. Theory of hyperbolic varieties. Arithmetical Kleinian and Fuchsian groups can be described in terms of maximal orders2. 1n is 2 in the cases of forms and the degree of the central simple algebra in that case. 2See for example, L.E. Arenas-Carmona, Representation fields for cyclic orders, Acta arithmetica, 156.2 (2012) 1 3. Theory of modular forms. Studying maximal orders in CSA's is one way to gen- eralize the classic theory of modular forms3. -
Chapter 19 the Clifford Algebra in the Theory of Algebras, Quadratic
This is page 307 Printer: Opaque this Chapter 19 The Clifford Algebra in the Theory of Algebras, Quadratic Forms, and Classical Groups Alexander Hahn1 ABSTRACT This article is an expanded version of my plenary lecture for the conference. It was the aim of the lecture to introduce the participants of the conference – their diverse realms of expertise ranged from theoretical physics, to computer science, to pure mathematics – to the algebraic matters of the title above. The basic texts listed in the references – note that this listing is by no means complete – serve as illustration of the rich and persistent interest in these topics and provide a reader with an opportunity to explore them in detail. Keywords: Clifford algebra, quadratic form, classical group, involutions, Clif- ford modules 1 Basic quadratic forms We will set the stage in very general terms. Let R be a commutative (and associative) ring with 1. A quadratic form in n variables over R is a homo- geneous polynomial of degree 2 p(X1,...,Xn)= X ai,j XiXj 1≤i,j≤n with coefficients ai,j in R. Two quadratic forms are equivalent if there is an invertible linear substitution of variables that transforms the one into the 1Many thanks go to Rafa l Ab lamowicz and John Ryan for their wonderful organiza- tional effort in bringing together in stimulating conversation scholars from all disciplines of the multifaceted reality that is the Clifford algebra. I wish to dedicate this article to the memory of one of them: Many of us will miss the dynamic mathematical and personal presence of Pertti Lounesto. -
Quaternion Algebras and Q 1.1. What Are Quaternion Algebras?
INTRODUCTION TO THE LOCAL-GLOBAL PRINCIPLE LIANG XIAO Abstract. This is the notes of a series lectures on local-global principle and quaternion algebras, given at Connecticut Summer School in Number Theory. 1. Day I: Quaternion Algebras and Qp 1.1. What are Quaternion Algebras? 1.1.1. Hamiltonian H. Recall that we setup mathematics in such a way starting with positive integers N and integers Z to build Q as its quotient field, and then defining R using several equivalent axioms, e.g. Dedekind cut, or as certain completions. After that, we introduced the field of complex numbers as C = R ⊕ Ri, satisfying i2 = −1. One of the most important theorem for complex numbers is the Fundamental Theorem of Algebra: all complex coefficients non-constant polynomials f(x) 2 C[x] has a zero. In other words, C is an algebraically closed field; so there is no bigger field than C that is finite dimensional as an R-vector space. (With the development of physics), Hamilton discovered that there is an \associative-but- non-commutative field” (called a skew field or a division algebra) H which is 4-dimensional over R: H = R ⊕ Ri ⊕ Rj ⊕ Rk = ai + bj + cj + dk a; b; c; d 2 R ; where the multiplication is R-linear and subject to the following rules: i2 = j2 = k2 = −1; ij = −ji = k; jk = −kj = i; and ki = −ik = j: This particular H is called the Hamiltonian quaternion. One simple presentation of H is: 2 2 H := Chi; ji i + 1; j + 1; ij + ji : Question 1.1.2.