The Quaternion Group As a Symmetry Group
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Subgroups of Division Rings in Characteristic Zero Are Characterized
Subgroups of Division Rings Mark Lewis Murray Schacher June 27, 2018 Abstract We investigate the finite subgroups that occur in the Hamiltonian quaternion algebra over the real subfield of cyclotomic fields. When possible, we investigate their distribution among the maximal orders. MSC(2010): Primary: 16A39, 12E15; Secondary: 16U60 1 Introduction Let F be a field, and fix a and b to be non-0 elements of F . The symbol algebra A =(a, b) is the 4-dimensional algebra over F generated by elements i and j that satisfy the relations: i2 = a, j2 = b, ij = ji. (1) − One usually sets k = ij, which leads to the additional circular relations ij = k = ji, jk = i = kj, ki = j = ki. (2) − − − arXiv:1806.09654v1 [math.RA] 25 Jun 2018 The set 1, i, j, k forms a basis for A over F . It is not difficult to see that A is a central{ simple} algebra over F , and using Wedderburn’s theorem, we see that A is either a 4-dimensional division ring or the ring M2(F ) of2 2 matrices over F . It is known that A is split (i.e. is the ring of 2 2 matrices× over F ) if and only if b is a norm from the field F (√a). Note that×b is a norm over F (√a) if and only if there exist elements x, y F so that b = x2 y2a. This condition is symmetric in a and b. ∈ − More generally, we have the following isomorphism of algebras: (a, b) ∼= (a, ub) (3) 1 where u = x2 y2a is a norm from F (√a); see [4] or [6]. -
Crystal Symmetry Groups
X-Ray and Neutron Crystallography rational numbers is a group under Crystal Symmetry Groups multiplication, and both it and the integer group already discussed are examples of infinite groups because they each contain an infinite number of elements. ymmetry plays an important role between the integers obey the rules of In the case of a symmetry group, in crystallography. The ways in group theory: an element is the operation needed to which atoms and molecules are ● There must be defined a procedure for produce one object from another. For arrangeds within a unit cell and unit cells example, a mirror operation takes an combining two elements of the group repeat within a crystal are governed by to form a third. For the integers one object in one location and produces symmetry rules. In ordinary life our can choose the addition operation so another of the opposite hand located first perception of symmetry is what that a + b = c is the operation to be such that the mirror doing the operation is known as mirror symmetry. Our performed and u, b, and c are always is equidistant between them (Fig. 1). bodies have, to a good approximation, elements of the group. These manipulations are usually called mirror symmetry in which our right side ● There exists an element of the group, symmetry operations. They are com- is matched by our left as if a mirror called the identity element and de- bined by applying them to an object se- passed along the central axis of our noted f, that combines with any other bodies. -
Generalized Quaternions
GENERALIZED QUATERNIONS KEITH CONRAD 1. introduction The quaternion group Q8 is one of the two non-abelian groups of size 8 (up to isomor- phism). The other one, D4, can be constructed as a semi-direct product: ∼ ∼ × ∼ D4 = Aff(Z=(4)) = Z=(4) o (Z=(4)) = Z=(4) o Z=(2); where the elements of Z=(2) act on Z=(4) as the identity and negation. While Q8 is not a semi-direct product, it can be constructed as the quotient group of a semi-direct product. We will see how this is done in Section2 and then jazz up the construction in Section3 to make an infinite family of similar groups with Q8 as the simplest member. In Section4 we will compare this family with the dihedral groups and see how it fits into a bigger picture. 2. The quaternion group from a semi-direct product The group Q8 is built out of its subgroups hii and hji with the overlapping condition i2 = j2 = −1 and the conjugacy relation jij−1 = −i = i−1. More generally, for odd a we have jaij−a = −i = i−1, while for even a we have jaij−a = i. We can combine these into the single formula a (2.1) jaij−a = i(−1) for all a 2 Z. These relations suggest the following way to construct the group Q8. Theorem 2.1. Let H = Z=(4) o Z=(4), where (a; b)(c; d) = (a + (−1)bc; b + d); ∼ The element (2; 2) in H has order 2, lies in the center, and H=h(2; 2)i = Q8. -
Molecular Symmetry
Molecular Symmetry 1 I. WHAT IS SYMMETRY AND WHY IT IS IMPORTANT? Some object are ”more symmetrical” than others. A sphere is more symmetrical than a cube because it looks the same after rotation through any angle about the diameter. A cube looks the same only if it is rotated through certain angels about specific axes, such as 90o, 180o, or 270o about an axis passing through the centers of any of its opposite faces, or by 120o or 240o about an axis passing through any of the opposite corners. Here are also examples of different molecules which remain the same after certain symme- try operations: NH3, H2O, C6H6, CBrClF . In general, an action which leaves the object looking the same after a transformation is called a symmetry operation. Typical symme- try operations include rotations, reflections, and inversions. There is a corresponding symmetry element for each symmetry operation, which is the point, line, or plane with respect to which the symmetry operation is performed. For instance, a rotation is carried out around an axis, a reflection is carried out in a plane, while an inversion is carried our in a point. We shall see that we can classify molecules that possess the same set of symmetry ele- ments, and grouping together molecules that possess the same set of symmetry elements. This classification is very important, because it allows to make some general conclusions about molecular properties without calculation. Particularly, we will be able to decide if a molecule has a dipole moment, or not and to know in advance the degeneracy of molecular states. -
Math.AG] 17 Mar 2001 Ebro Uhafml Mle H Og Ojcuefrinfin field 5-Dimensional for Such with Identify Type Conjecture to Weil Hope Hodge We of the Algebra
QUATERNIONIC PRYMS AND HODGE CLASSES B. VAN GEEMEN AND A. VERRA Abstract. Abelian varieties of dimension 2n on which a definite quaternion algebra acts are parametrized by symmetrical domains of dimension n(n 1)/2. Such abelian varieties have primitive Hodge classes in the middle dimensional cohomolo−gy group. In general, it is not clear that these are cycle classes. In this paper we show that a particular 6-dimensional family of such 8-folds are Prym varieties and we use the method of C. Schoen to show that all Hodge classes on the general abelian variety in this family are algebraic. We also consider Hodge classes on certain 5-dimensional subfamilies and relate these to the Hodge conjecture for abelian 4-folds. In this paper we study abelian varieties of dimension 8 whose endomorphism ring is a definite quaternion algebra over Q, we refer to these as abelian 8-folds of quaternion type. Such abelian varieties are interesting since their Hodge rings are not generated by divisor classes [M] and the Hodge conjecture is still open for most of them. The moduli space of 8-folds of quaternion type, with fixed discrete data, is 6-dimensional. One such moduli space was investigated recently by Freitag and Hermann [FrHe]. In [KSTT] a 6-dimensional family of K3 surfaces is studied whose Kuga-Satake varieties have simple factors of dimension 8 which are of quaternion type. Our first result, in section 3, is that one of these moduli spaces parametrizes Prym varieties of unramified 2:1 covers C˜ Cˆ, actually the genus 17 curves C˜ are 8:1 unramified covers of genus 3 curves with Galois→ group Q generated by the quaternions i and j. -
A Note on the Quaternion Group As Galois Group
proceedings of the american mathematical society Volume 108, Number 3, March 1990 A NOTE ON THE QUATERNION GROUP AS GALOIS GROUP ROGER WARE (Communicated by Louis J. Ratliff, Jr.) Abstract. The occurrence of the quaternion group as a Galois group over cer- tain fields is investigated. A theorem of Witt on quaternionic Galois extensions plays a key role. In [9, §6] Witt proved a theorem characterizing quaternionic Galois exten- sions. Namely, he showed that if F is a field of characteristic not 2 then an extension L = F(y/ä,y/b), a,b e F, of degree 4 over F can be embedded in a Galois extension A" of 7 with Gal(K/F) = 77g (the quaternion group 7 7 7 of order 8) if and only if the quadratic form ax + by + abz is isomorphic to x 2 + y 2 + z 2 .In addition he showed how to explicitly construct the Galois extension from the isometry. An immediate and interesting consequence of this is the fact that 77g cannot be a Galois group over any Pythagorean field. In this note Witt's theorem is used to obtain additional results about the existence of 77g as a Galois group over certain fields. If 7 is a field (of char- acteristic not 2) with at most one (total) ordering such that 77g does not oc- cur as a Galois group over F then the structure of the pro-2-Galois groups GF(2) = Gal(7(2)/7), Gpy = Gal(7py/7) (where 7(2) and Fpy are the quadratic and Pythagorean closures of F) are completely determined. -
A Classification of Clifford Algebras As Images of Group Algebras of Salingaros Vee Groups
DEPARTMENT OF MATHEMATICS TECHNICAL REPORT A CLASSIFICATION OF CLIFFORD ALGEBRAS AS IMAGES OF GROUP ALGEBRAS OF SALINGAROS VEE GROUPS R. Ablamowicz,M.Varahagiri,A.M.Walley November 2017 No. 2017-3 TENNESSEE TECHNOLOGICAL UNIVERSITY Cookeville, TN 38505 A Classification of Clifford Algebras as Images of Group Algebras of Salingaros Vee Groups Rafa lAb lamowicz, Manisha Varahagiri and Anne Marie Walley Abstract. The main objective of this work is to prove that every Clifford algebra C`p;q is R-isomorphic to a quotient of a group algebra R[Gp;q] modulo an ideal J = (1 + τ) where τ is a central element of order 2. p+q+1 Here, Gp;q is a 2-group of order 2 belonging to one of Salingaros isomorphism classes N2k−1;N2k; Ω2k−1; Ω2k or Sk. Thus, Clifford al- gebras C`p;q can be classified by Salingaros classes. Since the group algebras R[Gp;q] are Z2-graded and the ideal J is homogeneous, the quotient algebras R[G]=J are Z2-graded. In some instances, the isomor- ∼ phism R[G]=J = C`p;q is also Z2-graded. By Salingaros Theorem, the groups Gp;q in the classes N2k−1 and N2k are iterative central products of the dihedral group D8 and the quaternion group Q8, and so they are extra-special. The groups in the classes Ω2k−1 and Ω2k are central products of N2k−1 and N2k with C2 × C2, respectively. The groups in the class Sk are central products of N2k or N2k with C4. Two algorithms to factor any Gp;q into an internal central product, depending on the class, are given. -
Special Unitary Group - Wikipedia
Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Special unitary group In mathematics, the special unitary group of degree n, denoted SU( n), is the Lie group of n×n unitary matrices with determinant 1. (More general unitary matrices may have complex determinants with absolute value 1, rather than real 1 in the special case.) The group operation is matrix multiplication. The special unitary group is a subgroup of the unitary group U( n), consisting of all n×n unitary matrices. As a compact classical group, U( n) is the group that preserves the standard inner product on Cn.[nb 1] It is itself a subgroup of the general linear group, SU( n) ⊂ U( n) ⊂ GL( n, C). The SU( n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and SU(3) in quantum chromodynamics.[1] The simplest case, SU(1) , is the trivial group, having only a single element. The group SU(2) is isomorphic to the group of quaternions of norm 1, and is thus diffeomorphic to the 3-sphere. Since unit quaternions can be used to represent rotations in 3-dimensional space (up to sign), there is a surjective homomorphism from SU(2) to the rotation group SO(3) whose kernel is {+ I, − I}. [nb 2] SU(2) is also identical to one of the symmetry groups of spinors, Spin(3), that enables a spinor presentation of rotations. Contents Properties Lie algebra Fundamental representation Adjoint representation The group SU(2) Diffeomorphism with S 3 Isomorphism with unit quaternions Lie Algebra The group SU(3) Topology Representation theory Lie algebra Lie algebra structure Generalized special unitary group Example Important subgroups See also 1 of 10 2/22/2018, 8:54 PM Special unitary group - Wikipedia https://en.wikipedia.org/wiki/Special_unitary_group Remarks Notes References Properties The special unitary group SU( n) is a real Lie group (though not a complex Lie group). -
Chapter 1 Group and Symmetry
Chapter 1 Group and Symmetry 1.1 Introduction 1. A group (G) is a collection of elements that can ‘multiply’ and ‘di- vide’. The ‘multiplication’ ∗ is a binary operation that is associative but not necessarily commutative. Formally, the defining properties are: (a) if g1, g2 ∈ G, then g1 ∗ g2 ∈ G; (b) there is an identity e ∈ G so that g ∗ e = e ∗ g = g for every g ∈ G. The identity e is sometimes written as 1 or 1; (c) there is a unique inverse g−1 for every g ∈ G so that g ∗ g−1 = g−1 ∗ g = e. The multiplication rules of a group can be listed in a multiplication table, in which every group element occurs once and only once in every row and every column (prove this !) . For example, the following is the multiplication table of a group with four elements named Z4. e g1 g2 g3 e e g1 g2 g3 g1 g1 g2 g3 e g2 g2 g3 e g1 g3 g3 e g1 g2 Table 2.1 Multiplication table of Z4 3 4 CHAPTER 1. GROUP AND SYMMETRY 2. Two groups with identical multiplication tables are usually considered to be the same. We also say that these two groups are isomorphic. Group elements could be familiar mathematical objects, such as numbers, matrices, and differential operators. In that case group multiplication is usually the ordinary multiplication, but it could also be ordinary addition. In the latter case the inverse of g is simply −g, the identity e is simply 0, and the group multiplication is commutative. -
Some Properties of Representation of Quaternion Group
ICBSA 2018 International Conference on Basic Sciences and Its Applications Volume 2019 Conference Paper Some Properties of Representation of Quaternion Group Sri Rahayu, Maria Soviana, Yanita, and Admi Nazra Department of Mathematics, Andalas University, Limau Manis, Padang, 25163, Indonesia Abstract The quaternions are a number system in the form 푎 + 푏푖 + 푐푗 + 푑푘. The quaternions ±1, ±푖, ±푗, ±푘 form a non-abelian group of order eight called quaternion group. Quaternion group can be represented as a subgroup of the general linear group 퐺퐿2(C). In this paper, we discuss some group properties of representation of quaternion group related to Hamiltonian group, solvable group, nilpotent group, and metacyclic group. Keywords: representation of quaternion group, hamiltonian group, solvable group, nilpotent group, metacyclic group Corresponding Author: Sri Rahayu [email protected] Received: 19 February 2019 1. Introduction Accepted: 5 March 2019 Published: 16 April 2019 First we review that quaternion group, denoted by 푄8, was obtained based on the Publishing services provided by calculation of quaternions 푎 + 푏푖 + 푐푗 + 푑푘. Quaternions were first described by William Knowledge E Rowan Hamilton on October 1843 [1]. The quaternion group is a non-abelian group of Sri Rahayu et al. This article is order eight. distributed under the terms of the Creative Commons Attribution License, which 2. Materials and Methods permits unrestricted use and redistribution provided that the original author and source are Here we provide Definitions of quaternion group dan matrix representation. credited. Selection and Peer-review under Definition 1.1. [2] The quaternion group, 푄8, is defined by the responsibility of the ICBSA Conference Committee. -
Arxiv:1305.5974V1 [Math-Ph]
INTRODUCTION TO SPORADIC GROUPS for physicists Luis J. Boya∗ Departamento de F´ısica Te´orica Universidad de Zaragoza E-50009 Zaragoza, SPAIN MSC: 20D08, 20D05, 11F22 PACS numbers: 02.20.a, 02.20.Bb, 11.24.Yb Key words: Finite simple groups, sporadic groups, the Monster group. Juan SANCHO GUIMERA´ In Memoriam Abstract We describe the collection of finite simple groups, with a view on physical applications. We recall first the prime cyclic groups Zp, and the alternating groups Altn>4. After a quick revision of finite fields Fq, q = pf , with p prime, we consider the 16 families of finite simple groups of Lie type. There are also 26 extra “sporadic” groups, which gather in three interconnected “generations” (with 5+7+8 groups) plus the Pariah groups (6). We point out a couple of physical applications, in- cluding constructing the biggest sporadic group, the “Monster” group, with close to 1054 elements from arguments of physics, and also the relation of some Mathieu groups with compactification in string and M-theory. ∗[email protected] arXiv:1305.5974v1 [math-ph] 25 May 2013 1 Contents 1 Introduction 3 1.1 Generaldescriptionofthework . 3 1.2 Initialmathematics............................ 7 2 Generalities about groups 14 2.1 Elementarynotions............................ 14 2.2 Theframeworkorbox .......................... 16 2.3 Subgroups................................. 18 2.4 Morphisms ................................ 22 2.5 Extensions................................. 23 2.6 Familiesoffinitegroups ......................... 24 2.7 Abeliangroups .............................. 27 2.8 Symmetricgroup ............................. 28 3 More advanced group theory 30 3.1 Groupsoperationginspaces. 30 3.2 Representations.............................. 32 3.3 Characters.Fourierseries . 35 3.4 Homological algebra and extension theory . 37 3.5 Groupsuptoorder16.......................... -
Math 371 Review 1
Math 371 Review 1 Some Notation and Basic Concepts Linear Algebra fields. • Examples of fields: • { the field of rational, real and complex numbers: Q, R and C { Fp := the finite field with p elements, where p is a prime number { the field of rational functions, Q(x), R(x), C(x), consisting of quotients of poly- nomials with coefficients in Q, R, C respectively. vector spaces, subspaces. • dimension, basis, linear independence. • linear transformations (also called \homomorphisms between vector spaces") • matrix representations of a linear transformation. (So, after choosing a basis of the • source and a basis of a target vector space, a linear transformation is represented by a matrix.) Effect of change of bases on the matrix representation. direct sum of vector spaces • eigenvalues, eigenvectors, and eigenspaces (of a linear transformation), characteristic • polynomials. diagonalization (of a linear transformation) • Basic Grooup Theory groups, subgroups • Examples of groups • { cyclic groups: Z :=integers, Z=nZ = a cyclic group with n elements. { the dihedral group D2n with 2n elements; it is the group of all symmetries of a regular n-gon. { the quaternion group Q8 with 8 elements. { the \general linear groups" GLn(Q), GLn(R), GLn(C), GLn(Fp). These are the group of invertible n n matrices with coefficients in Q, R, C, and Fp respec- × tively. Notice that GL1(Q) = Q×, the group of non-zero rational numbers under multiplication; similarly GL1(R) = R×, GL1(C) = C×, GL1(Fp) = Fp×. 1 { the \special linear groups" SLn(Q), SLn(R), SLn(C) and SLn(Fp); each is the subgroup of the respective general linear group consisting of all elements whose determinant is equal to 1.