Generating Random Permutations
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An Exploration of the Relationship Between Mathematics and Music
An Exploration of the Relationship between Mathematics and Music Shah, Saloni 2010 MIMS EPrint: 2010.103 Manchester Institute for Mathematical Sciences School of Mathematics The University of Manchester Reports available from: http://eprints.maths.manchester.ac.uk/ And by contacting: The MIMS Secretary School of Mathematics The University of Manchester Manchester, M13 9PL, UK ISSN 1749-9097 An Exploration of ! Relation"ip Between Ma#ematics and Music MATH30000, 3rd Year Project Saloni Shah, ID 7177223 University of Manchester May 2010 Project Supervisor: Professor Roger Plymen ! 1 TABLE OF CONTENTS Preface! 3 1.0 Music and Mathematics: An Introduction to their Relationship! 6 2.0 Historical Connections Between Mathematics and Music! 9 2.1 Music Theorists and Mathematicians: Are they one in the same?! 9 2.2 Why are mathematicians so fascinated by music theory?! 15 3.0 The Mathematics of Music! 19 3.1 Pythagoras and the Theory of Music Intervals! 19 3.2 The Move Away From Pythagorean Scales! 29 3.3 Rameau Adds to the Discovery of Pythagoras! 32 3.4 Music and Fibonacci! 36 3.5 Circle of Fifths! 42 4.0 Messiaen: The Mathematics of his Musical Language! 45 4.1 Modes of Limited Transposition! 51 4.2 Non-retrogradable Rhythms! 58 5.0 Religious Symbolism and Mathematics in Music! 64 5.1 Numbers are God"s Tools! 65 5.2 Religious Symbolism and Numbers in Bach"s Music! 67 5.3 Messiaen"s Use of Mathematical Ideas to Convey Religious Ones! 73 6.0 Musical Mathematics: The Artistic Aspect of Mathematics! 76 6.1 Mathematics as Art! 78 6.2 Mathematical Periods! 81 6.3 Mathematics Periods vs. -
18.703 Modern Algebra, Permutation Groups
5. Permutation groups Definition 5.1. Let S be a set. A permutation of S is simply a bijection f : S −! S. Lemma 5.2. Let S be a set. (1) Let f and g be two permutations of S. Then the composition of f and g is a permutation of S. (2) Let f be a permutation of S. Then the inverse of f is a permu tation of S. Proof. Well-known. D Lemma 5.3. Let S be a set. The set of all permutations, under the operation of composition of permutations, forms a group A(S). Proof. (5.2) implies that the set of permutations is closed under com position of functions. We check the three axioms for a group. We already proved that composition of functions is associative. Let i: S −! S be the identity function from S to S. Let f be a permutation of S. Clearly f ◦ i = i ◦ f = f. Thus i acts as an identity. Let f be a permutation of S. Then the inverse g of f is a permutation of S by (5.2) and f ◦ g = g ◦ f = i, by definition. Thus inverses exist and G is a group. D Lemma 5.4. Let S be a finite set with n elements. Then A(S) has n! elements. Proof. Well-known. D Definition 5.5. The group Sn is the set of permutations of the first n natural numbers. We want a convenient way to represent an element of Sn. The first way, is to write an element σ of Sn as a matrix. -
Supplement on the Symmetric Group
SUPPLEMENT ON THE SYMMETRIC GROUP RUSS WOODROOFE I presented a couple of aspects of the theory of the symmetric group Sn differently than what is in Herstein. These notes will sketch this material. You will still want to read your notes and Herstein Chapter 2.10. 1. Conjugacy 1.1. The big idea. We recall from Linear Algebra that conjugacy in the matrix GLn(R) corresponds to changing basis in the underlying vector space n n R . Since GLn(R) is exactly the automorphism group of R (check the n definitions!), it’s equivalent to say that conjugation in Aut R corresponds n to change of basis in R . Similarly, Sn is Sym[n], the symmetries of the set [n] = {1, . , n}. We could think of an element of Sym[n] as being a “set automorphism” – this just says that sets have no interesting structure, unlike vector spaces with their abelian group structure. You might expect conjugation in Sn to correspond to some sort of change in basis of [n]. 1.2. Mathematical details. Lemma 1. Let g = (α1, . , αk) be a k-cycle in Sn, and h ∈ Sn be any element. Then h g = (α1 · h, α2 · h, . αk · h). h Proof. We show that g has the same action as (α1 · h, α2 · h, . αk · h), and since Sn acts faithfully (with trivial kernel) on [n], the lemma follows. h −1 First: (αi · h) · g = (αi · h) · h gh = αi · gh. If 1 ≤ i < m, then αi · gh = αi+1 · h as desired; otherwise αm · h = α1 · h also as desired. -
Permutation Group and Determinants (Dated: September 16, 2021)
Permutation group and determinants (Dated: September 16, 2021) 1 I. SYMMETRIES OF MANY-PARTICLE FUNCTIONS Since electrons are fermions, the electronic wave functions have to be antisymmetric. This chapter will show how to achieve this goal. The notion of antisymmetry is related to permutations of electrons’ coordinates. Therefore we will start with the discussion of the permutation group and then introduce the permutation-group-based definition of determinant, the zeroth-order approximation to the wave function in theory of many fermions. This definition, in contrast to that based on the Laplace expansion, relates clearly to properties of fermionic wave functions. The determinant gives an N-particle wave function built from a set of N one-particle waves functions and is called Slater’s determinant. II. PERMUTATION (SYMMETRIC) GROUP Definition of permutation group: The permutation group, known also under the name of symmetric group, is the group of all operations on a set of N distinct objects that order the objects in all possible ways. The group is denoted as SN (we will show that this is a group below). We will call these operations permutations and denote them by symbols σi. For a set consisting of numbers 1, 2, :::, N, the permutation σi orders these numbers in such a way that k is at jth position. Often a better way of looking at permutations is to say that permutations are all mappings of the set 1, 2, :::, N onto itself: σi(k) = j, where j has to go over all elements. Number of permutations: The number of permutations is N! Indeed, we can first place each object at positions 1, so there are N possible placements. -
Abstract Algebra
Abstract Algebra Paul Melvin Bryn Mawr College Fall 2011 lecture notes loosely based on Dummit and Foote's text Abstract Algebra (3rd ed) Prerequisite: Linear Algebra (203) 1 Introduction Pure Mathematics Algebra Analysis Foundations (set theory/logic) G eometry & Topology What is Algebra? • Number systems N = f1; 2; 3;::: g \natural numbers" Z = f:::; −1; 0; 1; 2;::: g \integers" Q = ffractionsg \rational numbers" R = fdecimalsg = pts on the line \real numbers" p C = fa + bi j a; b 2 R; i = −1g = pts in the plane \complex nos" k polar form re iθ, where a = r cos θ; b = r sin θ a + bi b r θ a p Note N ⊂ Z ⊂ Q ⊂ R ⊂ C (all proper inclusions, e.g. 2 62 Q; exercise) There are many other important number systems inside C. 2 • Structure \binary operations" + and · associative, commutative, and distributive properties \identity elements" 0 and 1 for + and · resp. 2 solve equations, e.g. 1 ax + bx + c = 0 has two (complex) solutions i p −b ± b2 − 4ac x = 2a 2 2 2 2 x + y = z has infinitely many solutions, even in N (thei \Pythagorian triples": (3,4,5), (5,12,13), . ). n n n 3 x + y = z has no solutions x; y; z 2 N for any fixed n ≥ 3 (Fermat'si Last Theorem, proved in 1995 by Andrew Wiles; we'll give a proof for n = 3 at end of semester). • Abstract systems groups, rings, fields, vector spaces, modules, . A group is a set G with an associative binary operation ∗ which has an identity element e (x ∗ e = x = e ∗ x for all x 2 G) and inverses for each of its elements (8 x 2 G; 9 y 2 G such that x ∗ y = y ∗ x = e). -
Parity Alternating Permutations Starting with an Odd Integer
Parity alternating permutations starting with an odd integer Frether Getachew Kebede1a, Fanja Rakotondrajaob aDepartment of Mathematics, College of Natural and Computational Sciences, Addis Ababa University, P.O.Box 1176, Addis Ababa, Ethiopia; e-mail: [email protected] bD´epartement de Math´ematiques et Informatique, BP 907 Universit´ed’Antananarivo, 101 Antananarivo, Madagascar; e-mail: [email protected] Abstract A Parity Alternating Permutation of the set [n] = 1, 2,...,n is a permutation with { } even and odd entries alternatively. We deal with parity alternating permutations having an odd entry in the first position, PAPs. We study the numbers that count the PAPs with even as well as odd parity. We also study a subclass of PAPs being derangements as well, Parity Alternating Derangements (PADs). Moreover, by considering the parity of these PADs we look into their statistical property of excedance. Keywords: parity, parity alternating permutation, parity alternating derangement, excedance 2020 MSC: 05A05, 05A15, 05A19 arXiv:2101.09125v1 [math.CO] 22 Jan 2021 1. Introduction and preliminaries A permutation π is a bijection from the set [n]= 1, 2,...,n to itself and we will write it { } in standard representation as π = π(1) π(2) π(n), or as the product of disjoint cycles. ··· The parity of a permutation π is defined as the parity of the number of transpositions (cycles of length two) in any representation of π as a product of transpositions. One 1Corresponding author. n c way of determining the parity of π is by obtaining the sign of ( 1) − , where c is the − number of cycles in the cycle representation of π. -
The Mathematics Major's Handbook
The Mathematics Major’s Handbook (updated Spring 2016) Mathematics Faculty and Their Areas of Expertise Jennifer Bowen Abstract Algebra, Nonassociative Rings and Algebras, Jordan Algebras James Hartman Linear Algebra, Magic Matrices, Involutions, (on leave) Statistics, Operator Theory Robert Kelvey Combinatorial and Geometric Group Theory Matthew Moynihan Abstract Algebra, Combinatorics, Permutation Enumeration R. Drew Pasteur Differential Equations, Mathematics in Biology/Medicine, Sports Data Analysis Pamela Pierce Real Analysis, Functions of Generalized Bounded Variation, Convergence of Fourier Series, Undergraduate Mathematics Education, Preparation of Pre-service Teachers John Ramsay Topology, Algebraic Topology, Operations Research OndˇrejZindulka Real Analysis, Fractal geometry, Geometric Measure Theory, Set Theory 1 2 Contents 1 Mission Statement and Learning Goals 5 1.1 Mathematics Department Mission Statement . 5 1.2 Learning Goals for the Mathematics Major . 5 2 Curriculum 8 3 Requirements for the Major 9 3.1 Recommended Timeline for the Mathematics Major . 10 3.2 Requirements for the Double Major . 10 3.3 Requirements for Teaching Licensure in Mathematics . 11 3.4 Requirements for the Minor . 11 4 Off-Campus Study in Mathematics 12 5 Senior Independent Study 13 5.1 Mathematics I.S. Student/Advisor Guidelines . 13 5.2 Project Topics . 13 5.3 Project Submissions . 14 5.3.1 Project Proposal . 14 5.3.2 Project Research . 14 5.3.3 Annotated Bibliography . 14 5.3.4 Thesis Outline . 15 5.3.5 Completed Chapters . 15 5.3.6 Digitial I.S. Document . 15 5.3.7 Poster . 15 5.3.8 Document Submission and oral presentation schedule . 15 6 Independent Study Assessment Guide 21 7 Further Learning Opportunities 23 7.1 At Wooster . -
Arxiv:2009.00554V2 [Math.CO] 10 Sep 2020 Graph On√ More Than Half of the Vertices of the D-Dimensional Hypercube Qd Has Maximum Degree at Least D
ON SENSITIVITY IN BIPARTITE CAYLEY GRAPHS IGNACIO GARCÍA-MARCO Facultad de Ciencias, Universidad de La Laguna, La Laguna, Spain KOLJA KNAUER∗ Aix Marseille Univ, Université de Toulon, CNRS, LIS, Marseille, France Departament de Matemàtiques i Informàtica, Universitat de Barcelona, Spain ABSTRACT. Huang proved that every set of more than halfp the vertices of the d-dimensional hyper- cube Qd induces a subgraph of maximum degree at least d, which is tight by a result of Chung, Füredi, Graham, and Seymour. Huang asked whether similar results can be obtained for other highly symmetric graphs. First, we present three infinite families of Cayley graphs of unbounded degree that contain in- duced subgraphs of maximum degree 1 on more than half the vertices. In particular, this refutes a conjecture of Potechin and Tsang, for which first counterexamples were shown recently by Lehner and Verret. The first family consists of dihedrants and contains a sporadic counterexample encoun- tered earlier by Lehner and Verret. The second family are star graphs, these are edge-transitive Cayley graphs of the symmetric group. All members of the third family are d-regular containing an d induced matching on a 2d−1 -fraction of the vertices. This is largest possible and answers a question of Lehner and Verret. Second, we consider Huang’s lower bound for graphs with subcubes and show that the corre- sponding lower bound is tight for products of Coxeter groups of type An, I2(2k + 1), and most exceptional cases. We believe that Coxeter groups are a suitable generalization of the hypercube with respect to Huang’s question. -
Universal Invariant and Equivariant Graph Neural Networks
Universal Invariant and Equivariant Graph Neural Networks Nicolas Keriven Gabriel Peyré École Normale Supérieure CNRS and École Normale Supérieure Paris, France Paris, France [email protected] [email protected] Abstract Graph Neural Networks (GNN) come in many flavors, but should always be either invariant (permutation of the nodes of the input graph does not affect the output) or equivariant (permutation of the input permutes the output). In this paper, we consider a specific class of invariant and equivariant networks, for which we prove new universality theorems. More precisely, we consider networks with a single hidden layer, obtained by summing channels formed by applying an equivariant linear operator, a pointwise non-linearity, and either an invariant or equivariant linear output layer. Recently, Maron et al. (2019b) showed that by allowing higher- order tensorization inside the network, universal invariant GNNs can be obtained. As a first contribution, we propose an alternative proof of this result, which relies on the Stone-Weierstrass theorem for algebra of real-valued functions. Our main contribution is then an extension of this result to the equivariant case, which appears in many practical applications but has been less studied from a theoretical point of view. The proof relies on a new generalized Stone-Weierstrass theorem for algebra of equivariant functions, which is of independent interest. Additionally, unlike many previous works that consider a fixed number of nodes, our results show that a GNN defined by a single set of parameters can approximate uniformly well a function defined on graphs of varying size. 1 Introduction Designing Neural Networks (NN) to exhibit some invariance or equivariance to group operations is a central problem in machine learning (Shawe-Taylor, 1993). -
Lecture 9: Permutation Groups
Lecture 9: Permutation Groups Prof. Dr. Ali Bülent EKIN· Doç. Dr. Elif TAN Ankara University Ali Bülent Ekin, Elif Tan (Ankara University) Permutation Groups 1 / 14 Permutation Groups Definition A permutation of a nonempty set A is a function s : A A that is one-to-one and onto. In other words, a pemutation of a set! is a rearrangement of the elements of the set. Theorem Let A be a nonempty set and let SA be the collection of all permutations of A. Then (SA, ) is a group, where is the function composition operation. The identity element of (SA, ) is the identity permutation i : A A, i (a) = a. ! 1 The inverse element of s is the permutation s such that 1 1 ss (a) = s s (a) = i (a) . Ali Bülent Ekin, Elif Tan (Ankara University) Permutation Groups 2 / 14 Permutation Groups Definition The group (SA, ) is called a permutation group on A. We will focus on permutation groups on finite sets. Definition Let In = 1, 2, ... , n , n 1 and let Sn be the set of all permutations on f g ≥ In.The group (Sn, ) is called the symmetric group on In. Let s be a permutation on In. It is convenient to use the following two-row notation: 1 2 n s = ··· s (1) s (2) s (n) ··· Ali Bülent Ekin, Elif Tan (Ankara University) Permutation Groups 3 / 14 Symmetric Groups 1 2 3 4 1 2 3 4 Example: Let f = and g = . Then 1 3 4 2 4 3 2 1 1 2 3 4 1 2 3 4 1 2 3 4 f g = = 1 3 4 2 4 3 2 1 2 4 3 1 1 2 3 4 1 2 3 4 1 2 3 4 g f = = 4 3 2 1 1 3 4 2 4 2 1 3 which shows that f g = g f . -
Notes on Finite Group Theory
Notes on finite group theory Peter J. Cameron October 2013 2 Preface Group theory is a central part of modern mathematics. Its origins lie in geome- try (where groups describe in a very detailed way the symmetries of geometric objects) and in the theory of polynomial equations (developed by Galois, who showed how to associate a finite group with any polynomial equation in such a way that the structure of the group encodes information about the process of solv- ing the equation). These notes are based on a Masters course I gave at Queen Mary, University of London. Of the two lecturers who preceded me, one had concentrated on finite soluble groups, the other on finite simple groups; I have tried to steer a middle course, while keeping finite groups as the focus. The notes do not in any sense form a textbook, even on finite group theory. Finite group theory has been enormously changed in the last few decades by the immense Classification of Finite Simple Groups. The most important structure theorem for finite groups is the Jordan–Holder¨ Theorem, which shows that any finite group is built up from finite simple groups. If the finite simple groups are the building blocks of finite group theory, then extension theory is the mortar that holds them together, so I have covered both of these topics in some detail: examples of simple groups are given (alternating groups and projective special linear groups), and extension theory (via factor sets) is developed for extensions of abelian groups. In a Masters course, it is not possible to assume that all the students have reached any given level of proficiency at group theory. -
Combinatorial Group Theory
Combinatorial Group Theory Charles F. Miller III 7 March, 2004 Abstract An early version of these notes was prepared for use by the participants in the Workshop on Algebra, Geometry and Topology held at the Australian National University, 22 January to 9 February, 1996. They have subsequently been updated and expanded many times for use by students in the subject 620-421 Combinatorial Group Theory at the University of Melbourne. Copyright 1996-2004 by C. F. Miller III. Contents 1 Preliminaries 3 1.1 About groups . 3 1.2 About fundamental groups and covering spaces . 5 2 Free groups and presentations 11 2.1 Free groups . 12 2.2 Presentations by generators and relations . 16 2.3 Dehn’s fundamental problems . 19 2.4 Homomorphisms . 20 2.5 Presentations and fundamental groups . 22 2.6 Tietze transformations . 24 2.7 Extraction principles . 27 3 Construction of new groups 30 3.1 Direct products . 30 3.2 Free products . 32 3.3 Free products with amalgamation . 36 3.4 HNN extensions . 43 3.5 HNN related to amalgams . 48 3.6 Semi-direct products and wreath products . 50 4 Properties, embeddings and examples 53 4.1 Countable groups embed in 2-generator groups . 53 4.2 Non-finite presentability of subgroups . 56 4.3 Hopfian and residually finite groups . 58 4.4 Local and poly properties . 61 4.5 Finitely presented coherent by cyclic groups . 63 1 5 Subgroup Theory 68 5.1 Subgroups of Free Groups . 68 5.1.1 The general case . 68 5.1.2 Finitely generated subgroups of free groups .