Octonionic Geometry
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The Enigmatic Number E: a History in Verse and Its Uses in the Mathematics Classroom
To appear in MAA Loci: Convergence The Enigmatic Number e: A History in Verse and Its Uses in the Mathematics Classroom Sarah Glaz Department of Mathematics University of Connecticut Storrs, CT 06269 [email protected] Introduction In this article we present a history of e in verse—an annotated poem: The Enigmatic Number e . The annotation consists of hyperlinks leading to biographies of the mathematicians appearing in the poem, and to explanations of the mathematical notions and ideas presented in the poem. The intention is to celebrate the history of this venerable number in verse, and to put the mathematical ideas connected with it in historical and artistic context. The poem may also be used by educators in any mathematics course in which the number e appears, and those are as varied as e's multifaceted history. The sections following the poem provide suggestions and resources for the use of the poem as a pedagogical tool in a variety of mathematics courses. They also place these suggestions in the context of other efforts made by educators in this direction by briefly outlining the uses of historical mathematical poems for teaching mathematics at high-school and college level. Historical Background The number e is a newcomer to the mathematical pantheon of numbers denoted by letters: it made several indirect appearances in the 17 th and 18 th centuries, and acquired its letter designation only in 1731. Our history of e starts with John Napier (1550-1617) who defined logarithms through a process called dynamical analogy [1]. Napier aimed to simplify multiplication (and in the same time also simplify division and exponentiation), by finding a model which transforms multiplication into addition. -
Irrational Numbers Unit 4 Lesson 6 IRRATIONAL NUMBERS
Irrational Numbers Unit 4 Lesson 6 IRRATIONAL NUMBERS Students will be able to: Understand the meanings of Irrational Numbers Key Vocabulary: • Irrational Numbers • Examples of Rational Numbers and Irrational Numbers • Decimal expansion of Irrational Numbers • Steps for representing Irrational Numbers on number line IRRATIONAL NUMBERS A rational number is a number that can be expressed as a ratio or we can say that written as a fraction. Every whole number is a rational number, because any whole number can be written as a fraction. Numbers that are not rational are called irrational numbers. An Irrational Number is a real number that cannot be written as a simple fraction or we can say cannot be written as a ratio of two integers. The set of real numbers consists of the union of the rational and irrational numbers. If a whole number is not a perfect square, then its square root is irrational. For example, 2 is not a perfect square, and √2 is irrational. EXAMPLES OF RATIONAL NUMBERS AND IRRATIONAL NUMBERS Examples of Rational Number The number 7 is a rational number because it can be written as the 7 fraction . 1 The number 0.1111111….(1 is repeating) is also rational number 1 because it can be written as fraction . 9 EXAMPLES OF RATIONAL NUMBERS AND IRRATIONAL NUMBERS Examples of Irrational Numbers The square root of 2 is an irrational number because it cannot be written as a fraction √2 = 1.4142135…… Pi(휋) is also an irrational number. π = 3.1415926535897932384626433832795 (and more...) 22 The approx. value of = 3.1428571428571.. -
Generically Split Octonion Algebras and A1-Homotopy Theory
Generically split octonion algebras and A1-homotopy theory Aravind Asok∗ Marc Hoyoisy Matthias Wendtz Abstract 1 We study generically split octonion algebras over schemes using techniques of A -homotopy theory. By combining affine representability results with techniques of obstruction theory, we establish classifica- tion results over smooth affine schemes of small dimension. In particular, for smooth affine schemes over algebraically closed fields, we show that generically split octonion algebras may be classified by charac- teristic classes including the second Chern class and another “mod 3” invariant. We review Zorn’s “vector matrix” construction of octonion algebras, generalized to rings by various authors, and show that generi- cally split octonion algebras are always obtained from this construction over smooth affine schemes of low dimension. Finally, generalizing P. Gille’s analysis of octonion algebras with trivial norm form, we observe that generically split octonion algebras with trivial associated spinor bundle are automatically split in low dimensions. Contents 1 Introduction 1 2 Octonion algebras, algebra and geometry 6 2.1 Octonion algebras and Zorn’s vector matrices......................................7 2.2 Octonion algebras and G2-torsors............................................9 2.3 Homogeneous spaces related to G2 and octonions.................................... 11 1 3 A -homotopy sheaves of BNis G2 17 1 3.1 Some A -fiber sequences................................................. 17 1 3.2 Characteristic maps and strictly A -invariant sheaves.................................. 19 3.3 Realization and characteristic maps........................................... 21 1 3.4 Some low degree A -homotopy sheaves of BNis Spinn and BNis G2 .......................... 24 4 Classifying octonion algebras 29 4.1 Classifying generically split octonion algebras...................................... 30 4.2 When are octonion algebras isomorphic to Zorn algebras?............................... -
Hypercomplex Algebras and Their Application to the Mathematical
Hypercomplex Algebras and their application to the mathematical formulation of Quantum Theory Torsten Hertig I1, Philip H¨ohmann II2, Ralf Otte I3 I tecData AG Bahnhofsstrasse 114, CH-9240 Uzwil, Schweiz 1 [email protected] 3 [email protected] II info-key GmbH & Co. KG Heinz-Fangman-Straße 2, DE-42287 Wuppertal, Deutschland 2 [email protected] March 31, 2014 Abstract Quantum theory (QT) which is one of the basic theories of physics, namely in terms of ERWIN SCHRODINGER¨ ’s 1926 wave functions in general requires the field C of the complex numbers to be formulated. However, even the complex-valued description soon turned out to be insufficient. Incorporating EINSTEIN’s theory of Special Relativity (SR) (SCHRODINGER¨ , OSKAR KLEIN, WALTER GORDON, 1926, PAUL DIRAC 1928) leads to an equation which requires some coefficients which can neither be real nor complex but rather must be hypercomplex. It is conventional to write down the DIRAC equation using pairwise anti-commuting matrices. However, a unitary ring of square matrices is a hypercomplex algebra by definition, namely an associative one. However, it is the algebraic properties of the elements and their relations to one another, rather than their precise form as matrices which is important. This encourages us to replace the matrix formulation by a more symbolic one of the single elements as linear combinations of some basis elements. In the case of the DIRAC equation, these elements are called biquaternions, also known as quaternions over the complex numbers. As an algebra over R, the biquaternions are eight-dimensional; as subalgebras, this algebra contains the division ring H of the quaternions at one hand and the algebra C ⊗ C of the bicomplex numbers at the other, the latter being commutative in contrast to H. -
Gauging the Octonion Algebra
UM-P-92/60_» Gauging the octonion algebra A.K. Waldron and G.C. Joshi Research Centre for High Energy Physics, University of Melbourne, Parkville, Victoria 8052, Australia By considering representation theory for non-associative algebras we construct the fundamental and adjoint representations of the octonion algebra. We then show how these representations by associative matrices allow a consistent octonionic gauge theory to be realized. We find that non-associativity implies the existence of new terms in the transformation laws of fields and the kinetic term of an octonionic Lagrangian. PACS numbers: 11.30.Ly, 12.10.Dm, 12.40.-y. Typeset Using REVTEX 1 L INTRODUCTION The aim of this work is to genuinely gauge the octonion algebra as opposed to relating properties of this algebra back to the well known theory of Lie Groups and fibre bundles. Typically most attempts to utilise the octonion symmetry in physics have revolved around considerations of the automorphism group G2 of the octonions and Jordan matrix representations of the octonions [1]. Our approach is more simple since we provide a spinorial approach to the octonion symmetry. Previous to this work there were already several indications that this should be possible. To begin with the statement of the gauge principle itself uno theory shall depend on the labelling of the internal symmetry space coordinates" seems to be independent of the exact nature of the gauge algebra and so should apply equally to non-associative algebras. The octonion algebra is an alternative algebra (the associator {x-1,y,i} = 0 always) X -1 so that the transformation law for a gauge field TM —• T^, = UY^U~ — ^(c^C/)(/ is well defined for octonionic transformations U. -
O/Zp OCTONION ALGEBRA and ITS MATRIX REPRESENTATIONS
Palestine Journal of Mathematics Vol. 6(1)(2017) , 307313 © Palestine Polytechnic University-PPU 2017 O Z OCTONION ALGEBRA AND ITS MATRIX = p REPRESENTATIONS Serpil HALICI and Adnan KARATA¸S Communicated by Ayman Badawi MSC 2010 Classications: Primary 17A20; Secondary 16G99. Keywords and phrases: Quaternion algebra, Octonion algebra, Cayley-Dickson process, Matrix representation. Abstract. Since O is a non-associative algebra over R, this real division algebra can not be algebraically isomorphic to any matrix algebras over the real number eld R. In this study using H with Cayley-Dickson process we obtain octonion algebra. Firstly, We investigate octonion algebra over Zp. Then, we use the left and right matrix representations of H to construct repre- sentation for octonion algebra. Furthermore, we get the matrix representations of O Z with the = p help of Cayley-Dickson process. 1 Introduction Let us summarize the notations needed to understand octonionic algebra. There are only four normed division algebras R, C, H and O [2], [6]. The octonion algebra is a non-commutative, non-associative but alternative algebra which discovered in 1843 by John T. Graves. Octonions have many applications in quantum logic, special relativity, supersymmetry, etc. Due to the non-associativity, representing octonions by matrices seems impossible. Nevertheless, one can overcome these problems by introducing left (or right) octonionic operators and xing the direc- tion of action. In this study we investigate matrix representations of octonion division algebra O Z . Now, lets = p start with the quaternion algebra H to construct the octonion algebra O. It is well known that any octonion a can be written by the Cayley-Dickson process as follows [7]. -
0.999… = 1 an Infinitesimal Explanation Bryan Dawson
0 1 2 0.9999999999999999 0.999… = 1 An Infinitesimal Explanation Bryan Dawson know the proofs, but I still don’t What exactly does that mean? Just as real num- believe it.” Those words were uttered bers have decimal expansions, with one digit for each to me by a very good undergraduate integer power of 10, so do hyperreal numbers. But the mathematics major regarding hyperreals contain “infinite integers,” so there are digits This fact is possibly the most-argued- representing not just (the 237th digit past “Iabout result of arithmetic, one that can evoke great the decimal point) and (the 12,598th digit), passion. But why? but also (the Yth digit past the decimal point), According to Robert Ely [2] (see also Tall and where is a negative infinite hyperreal integer. Vinner [4]), the answer for some students lies in their We have four 0s followed by a 1 in intuition about the infinitely small: While they may the fifth decimal place, and also where understand that the difference between and 1 is represents zeros, followed by a 1 in the Yth less than any positive real number, they still perceive a decimal place. (Since we’ll see later that not all infinite nonzero but infinitely small difference—an infinitesimal hyperreal integers are equal, a more precise, but also difference—between the two. And it’s not just uglier, notation would be students; most professional mathematicians have not or formally studied infinitesimals and their larger setting, the hyperreal numbers, and as a result sometimes Confused? Perhaps a little background information wonder . -
Arxiv:2012.09644V1 [Math.RA] 15 Dec 2020 Oitv -Iesoa Rs.Nnsoitv -Iesoa)Comp Form 8-Dimensional) Norm Nonassociative Associated Whose (Resp
SPLITTING OF QUATERNIONS AND OCTONIONS OVER PURELY INSEPARABLE EXTENSIONS IN CHARACTERISTIC 2 DETLEV W. HOFFMANN Abstract. We give examples of quaternion and octonion division algebras over a field F of characteristic 2 that split over a purely inseparable extension E of F of degree 4 but that do not split over any subextension of F inside E of lower exponent,≥ or, in the case of octonions, over any simple subextension of F inside E. Thus, we get a negative answer to a question posed by Bernhard M¨uhlherr and Richard Weiss. We study this question in terms of the isotropy behaviour of the associated norm forms. 1. Introduction Recall that a quaternion (resp. octonion) algebra A over a field F is a an as- sociative 4-dimensional (resp. nonassociative 8-dimensional) composition algebra whose associated norm form nA is a nondegenerate quadratic form defined on the F -vector space A. This norm form has the property that A is a division algebra iff nA is anisotropic. Furthermore, nA determines A in the sense that if A′ is an- other quaternion (resp. octonion) algebra, then A ∼= A′ as F -algebras iff nA ∼= nA′ (i.e., the norm forms are isometric). There is a vast amount of literature on such algebras. In this note, we consider only base fields of characteristic 2, a case that, compared to characteristic not 2, gives rise to additional subtleties that make the theory in some sense richer but also more intricate and complicated. For example, when conisdering subfields of such algebras one has to distingush between separable and inseparable quadratic extensions. -
1.1 the Real Number System
1.1 The Real Number System Types of Numbers: The following diagram shows the types of numbers that form the set of real numbers. Definitions 1. The natural numbers are the numbers used for counting. 1, 2, 3, 4, 5, . A natural number is a prime number if it is greater than 1 and its only factors are 1 and itself. A natural number is a composite number if it is greater than 1 and it is not prime. Example: 5, 7, 13,29, 31 are prime numbers. 8, 24, 33 are composite numbers. 2. The whole numbers are the natural numbers and zero. 0, 1, 2, 3, 4, 5, . 3. The integers are all the whole numbers and their additive inverses. No fractions or decimals. , -3, -2, -1, 0, 1, 2, 3, . An integer is even if it can be written in the form 2n , where n is an integer (if 2 is a factor). An integer is odd if it can be written in the form 2n −1, where n is an integer (if 2 is not a factor). Example: 2, 0, 8, -24 are even integers and 1, 57, -13 are odd integers. 4. The rational numbers are the numbers that can be written as the ratio of two integers. All rational numbers when written in their equivalent decimal form will have terminating or repeating decimals. 1 2 , 3.25, 0.8125252525 …, 0.6 , 2 ( = ) 5 1 1 5. The irrational numbers are any real numbers that can not be represented as the ratio of two integers. -
On H(X)-Fibonacci Octonion Polynomials, Ahmet Ipek & Kamil
Alabama Journal of Mathematics ISSN 2373-0404 39 (2015) On h(x)-Fibonacci octonion polynomials Ahmet Ipek˙ Kamil Arı Karamanoglu˘ Mehmetbey University, Karamanoglu˘ Mehmetbey University, Science Faculty of Kamil Özdag,˘ Science Faculty of Kamil Özdag,˘ Department of Mathematics, Karaman, Turkey Department of Mathematics, Karaman, Turkey In this paper, we introduce h(x)-Fibonacci octonion polynomials that generalize both Cata- lan’s Fibonacci octonion polynomials and Byrd’s Fibonacci octonion polynomials and also k- Fibonacci octonion numbers that generalize Fibonacci octonion numbers. Also we derive the Binet formula and and generating function of h(x)-Fibonacci octonion polynomial sequence. Introduction and Lucas numbers (Tasci and Kilic (2004)). Kiliç et al. (2006) gave the Binet formula for the generalized Pell se- To investigate the normed division algebras is greatly a quence. important topic today. It is well known that the octonions The investigation of special number sequences over H and O are the nonassociative, noncommutative, normed division O which are not analogs of ones over R and C has attracted algebra over the real numbers R. Due to the nonassociative some recent attention (see, e.g.,Akyigit,˘ Kösal, and Tosun and noncommutativity, one cannot directly extend various re- (2013), Halici (2012), Halici (2013), Iyer (1969), A. F. Ho- sults on real, complex and quaternion numbers to octonions. radam (1963) and Keçilioglu˘ and Akkus (2015)). While ma- The book by Conway and Smith (n.d.) gives a great deal of jority of papers in the area are devoted to some Fibonacci- useful background on octonions, much of it based on the pa- type special number sequences over R and C, only few of per of Coxeter et al. -
Computability on the Real Numbers
4. Computability on the Real Numbers Real numbers are the basic objects in analysis. For most non-mathematicians a real number is an infinite decimal fraction, for example π = 3•14159 ... Mathematicians prefer to define the real numbers axiomatically as follows: · (R, +, , 0, 1,<) is, up to isomorphism, the only Archimedean ordered field satisfying the axiom of continuity [Die60]. The set of real numbers can also be constructed in various ways, for example by means of Dedekind cuts or by completion of the (metric space of) rational numbers. We will neglect all foundational problems and assume that the real numbers form a well-defined set R with all the properties which are proved in analysis. We will denote the R real line topology, that is, the set of all open subsets of ,byτR. In Sect. 4.1 we introduce several representations of the real numbers, three of which (and the equivalent ones) will survive as useful. We introduce a rep- n n resentation ρ of R by generalizing the definition of the main representation ρ of the set R of real numbers. In Sect. 4.2 we discuss the computable real numbers. Sect. 4.3 is devoted to computable real functions. We show that many well known functions are computable, and we show that partial sum- mation of sequences is computable and that limit operator on sequences of real numbers is computable, if a modulus of convergence is given. We also prove a computability theorem for power series. Convention 4.0.1. We still assume that Σ is a fixed finite alphabet con- taining all the symbols we will need. -
1 the Real Number Line
Unit 2 Real Number Line and Variables Lecture Notes Introductory Algebra Page 1 of 13 1 The Real Number Line There are many sets of numbers, but important ones in math and life sciences are the following • The integers Z = f:::; −4; −3; −2; −1; 0; 1; 2; 3; 4;:::g. • The positive integers, sometimes called natural numbers, N = f1; 2; 3; 4;:::g. p • Rational numbers are any number that can be expressed as a fraction where p and q 6= 0 are integers. Q q Note that every integer is a rational number! • An irrational number is a number that is not rational. p Examples of irrational numbers are 2 ∼ 1:41421 :::, e ∼ 2:71828 :::, π ∼ 3:14159265359 :::, and less familiar ones like Euler's constant γ ∼ 0:577215664901532 :::. The \:::" here represent that the number is a nonrepeating, nonterminating decimal. • The real numbers R contain all the integer number, rational numbers, and irrational numbers. The real numbers are usually presented as a real number line, which extends forever to the left and right. Note the real numbers are not bounded above or below. To indicate that the real number line extends forever in the positive direction, we use the terminology infinity, which is written as 1, and in the negative direction the real number line extends to minus infinity, which is denoted −∞. The symbol 1 is used to say that the real numbers extend without bound (for any real number, there is a larger real number and a smaller real number). Infinity is a somewhat tricky concept, and you will learn more about it in precalculus and calculus.