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Projective Planarity of Matroids of 3-Nets and Biased Graphs
AUSTRALASIAN JOURNAL OF COMBINATORICS Volume 76(2) (2020), Pages 299–338 Projective planarity of matroids of 3-nets and biased graphs Rigoberto Florez´ ∗ Deptartment of Mathematical Sciences, The Citadel Charleston, South Carolina 29409 U.S.A. [email protected] Thomas Zaslavsky† Department of Mathematical Sciences, Binghamton University Binghamton, New York 13902-6000 U.S.A. [email protected] Abstract A biased graph is a graph with a class of selected circles (“cycles”, “cir- cuits”), called “balanced”, such that no theta subgraph contains exactly two balanced circles. A 3-node biased graph is equivalent to an abstract partial 3-net. We work in terms of a special kind of 3-node biased graph called a biased expansion of a triangle. Our results apply to all finite 3-node biased graphs because, as we prove, every such biased graph is a subgraph of a finite biased expansion of a triangle. A biased expansion of a triangle is equivalent to a 3-net, which, in turn, is equivalent to an isostrophe class of quasigroups. A biased graph has two natural matroids, the frame matroid and the lift matroid. A classical question in matroid theory is whether a matroid can be embedded in a projective geometry. There is no known general answer, but for matroids of biased graphs it is possible to give algebraic criteria. Zaslavsky has previously given such criteria for embeddability of biased-graphic matroids in Desarguesian projective spaces; in this paper we establish criteria for the remaining case, that is, embeddability in an arbitrary projective plane that is not necessarily Desarguesian. -
Octonion Multiplication and Heawood's
CONFLUENTES MATHEMATICI Bruno SÉVENNEC Octonion multiplication and Heawood’s map Tome 5, no 2 (2013), p. 71-76. <http://cml.cedram.org/item?id=CML_2013__5_2_71_0> © Les auteurs et Confluentes Mathematici, 2013. Tous droits réservés. L’accès aux articles de la revue « Confluentes Mathematici » (http://cml.cedram.org/), implique l’accord avec les condi- tions générales d’utilisation (http://cml.cedram.org/legal/). Toute reproduction en tout ou partie de cet article sous quelque forme que ce soit pour tout usage autre que l’utilisation á fin strictement personnelle du copiste est constitutive d’une infrac- tion pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ Confluentes Math. 5, 2 (2013) 71-76 OCTONION MULTIPLICATION AND HEAWOOD’S MAP BRUNO SÉVENNEC Abstract. In this note, the octonion multiplication table is recovered from a regular tesse- lation of the equilateral two timensional torus by seven hexagons, also known as Heawood’s map. Almost any article or book dealing with Cayley-Graves algebra O of octonions (to be recalled shortly) has a picture like the following Figure 0.1 representing the so-called ‘Fano plane’, which will be denoted by Π, together with some cyclic ordering on each of its ‘lines’. The Fano plane is a set of seven points, in which seven three-point subsets called ‘lines’ are specified, such that any two points are contained in a unique line, and any two lines intersect in a unique point, giving a so-called (combinatorial) projective plane [8,7]. -
Matroids You Have Known
26 MATHEMATICS MAGAZINE Matroids You Have Known DAVID L. NEEL Seattle University Seattle, Washington 98122 [email protected] NANCY ANN NEUDAUER Pacific University Forest Grove, Oregon 97116 nancy@pacificu.edu Anyone who has worked with matroids has come away with the conviction that matroids are one of the richest and most useful ideas of our day. —Gian Carlo Rota [10] Why matroids? Have you noticed hidden connections between seemingly unrelated mathematical ideas? Strange that finding roots of polynomials can tell us important things about how to solve certain ordinary differential equations, or that computing a determinant would have anything to do with finding solutions to a linear system of equations. But this is one of the charming features of mathematics—that disparate objects share similar traits. Properties like independence appear in many contexts. Do you find independence everywhere you look? In 1933, three Harvard Junior Fellows unified this recurring theme in mathematics by defining a new mathematical object that they dubbed matroid [4]. Matroids are everywhere, if only we knew how to look. What led those junior-fellows to matroids? The same thing that will lead us: Ma- troids arise from shared behaviors of vector spaces and graphs. We explore this natural motivation for the matroid through two examples and consider how properties of in- dependence surface. We first consider the two matroids arising from these examples, and later introduce three more that are probably less familiar. Delving deeper, we can find matroids in arrangements of hyperplanes, configurations of points, and geometric lattices, if your tastes run in that direction. -
Latin Square Design and Incomplete Block Design Latin Square (LS) Design Latin Square (LS) Design
Lecture 8 Latin Square Design and Incomplete Block Design Latin Square (LS) design Latin square (LS) design • It is a kind of complete block designs. • A class of experimental designs that allow for two sources of blocking. • Can be constructed for any number of treatments, but there is a cost. If there are t treatments, then t2 experimental units will be required. Latin square design • If you can block on two (perpendicular) sources of variation (rows x columns) you can reduce experimental error when compared to the RBD • More restrictive than the RBD • The total number of plots is the square of the number of treatments • Each treatment appears once and only once in each row and column A B C D B C D A C D A B D A B C Facts about the LS Design • With the Latin Square design you are able to control variation in two directions. • Treatments are arranged in rows and columns • Each row contains every treatment. • Each column contains every treatment. • The most common sizes of LS are 5x5 to 8x8 Advantages • You can control variation in two directions. • Hopefully you increase efficiency as compared to the RBD. Disadvantages • The number of treatments must equal the number of replicates. • The experimental error is likely to increase with the size of the square. • Small squares have very few degrees of freedom for experimental error. • You can’t evaluate interactions between: • Rows and columns • Rows and treatments • Columns and treatments. Examples of Uses of the Latin Square Design • 1. Field trials in which the experimental error has two fertility gradients running perpendicular each other or has a unidirectional fertility gradient but also has residual effects from previous trials. -
The Turan Number of the Fano Plane
Combinatorica (5) (2005) 561–574 COMBINATORICA 25 Bolyai Society – Springer-Verlag THE TURAN´ NUMBER OF THE FANO PLANE PETER KEEVASH, BENNY SUDAKOV* Received September 17, 2002 Let PG2(2) be the Fano plane, i.e., the unique hypergraph with 7 triples on 7 vertices in which every pair of vertices is contained in a unique triple. In this paper we prove that for sufficiently large n, the maximum number of edges in a 3-uniform hypergraph on n vertices not containing a Fano plane is n n/2 n/2 ex n, P G (2) = − − . 2 3 3 3 Moreover, the only extremal configuration can be obtained by partitioning an n-element set into two almost equal parts, and taking all the triples that intersect both of them. This extends an earlier result of de Caen and F¨uredi, and proves an old conjecture of V. S´os. In addition, we also prove a stability result for the Fano plane, which says that a 3-uniform hypergraph with density close to 3/4 and no Fano plane is approximately 2-colorable. 1. Introduction Given an r-uniform hypergraph F,theTur´an number of F is the maximum number of edges in an r-uniform hypergraph on n vertices that does not contain a copy of F. We denote this number by ex(n,F). Determining these numbers is one of the central problems in Extremal Combinatorics, and it is well understood for ordinary graphs (the case r =2). It is completely solved for many instances, including all complete graphs. Moreover, asymptotic results are known for all non-bipartite graphs. -
Finite Projective Geometry 2Nd Year Group Project
Finite Projective Geometry 2nd year group project. B. Doyle, B. Voce, W.C Lim, C.H Lo Mathematics Department - Imperial College London Supervisor: Ambrus Pal´ June 7, 2015 Abstract The Fano plane has a strong claim on being the simplest symmetrical object with inbuilt mathematical structure in the universe. This is due to the fact that it is the smallest possible projective plane; a set of points with a subsets of lines satisfying just three axioms. We will begin by developing some theory direct from the axioms and uncovering some of the hidden (and not so hidden) symmetries of the Fano plane. Alternatively, some projective planes can be derived from vector space theory and we shall also explore this and the associated linear maps on these spaces. Finally, with the help of some theory of quadratic forms we will give a proof of the surprising Bruck-Ryser theorem, which shows that if a projective plane has order n congruent to 1 or 2 mod 4, then n is the sum of two squares. Thus we will have demonstrated fascinating links between pure mathematical disciplines by incorporating the use of linear algebra, group the- ory and number theory to explain the geometric world of projective planes. 1 Contents 1 Introduction 3 2 Basic Defintions and results 4 3 The Fano Plane 7 3.1 Isomorphism and Automorphism . 8 3.2 Ovals . 10 4 Projective Geometry with fields 12 4.1 Constructing Projective Planes from fields . 12 4.2 Order of Projective Planes over fields . 14 5 Bruck-Ryser 17 A Appendix - Rings and Fields 22 2 1 Introduction Projective planes are geometrical objects that consist of a set of elements called points and sub- sets of these elements called lines constructed following three basic axioms which give the re- sulting object a remarkable level of symmetry. -
Latin Squares in Experimental Design
Latin Squares in Experimental Design Lei Gao Michigan State University December 10, 2005 Abstract: For the past three decades, Latin Squares techniques have been widely used in many statistical applications. Much effort has been devoted to Latin Square Design. In this paper, I introduce the mathematical properties of Latin squares and the application of Latin squares in experimental design. Some examples and SAS codes are provided that illustrates these methods. Work done in partial fulfillment of the requirements of Michigan State University MTH 880 advised by Professor J. Hall. 1 Index Index ............................................................................................................................... 2 1. Introduction................................................................................................................. 3 1.1 Latin square........................................................................................................... 3 1.2 Orthogonal array representation ........................................................................... 3 1.3 Equivalence classes of Latin squares.................................................................... 3 2. Latin Square Design.................................................................................................... 4 2.1 Latin square design ............................................................................................... 4 2.2 Pros and cons of Latin square design................................................................... -
Weak Orientability of Matroids and Polynomial Equations
WEAK ORIENTABILITY OF MATROIDS AND POLYNOMIAL EQUATIONS J.A. DE LOERA1, J. LEE2, S. MARGULIES3, AND J. MILLER4 Abstract. This paper studies systems of polynomial equations that provide information about orientability of matroids. First, we study systems of linear equations over F2, originally alluded to by Bland and Jensen in their seminal paper on weak orientability. The Bland-Jensen linear equations for a matroid M have a solution if and only if M is weakly orientable. We use the Bland-Jensen system to determine weak orientability for all matroids on at most nine elements and all matroids between ten and twelve elements having rank three. Our experiments indicate that for small rank, about half the time, when a simple matroid is not orientable, it is already non-weakly orientable, and further this may happen more often as the rank increases. Thus, about half of the small simple non-orientable matroids of rank three are not representable over fields having order congruent to three modulo four. For binary matroids, the Bland-Jensen linear systems provide a practical way to check orientability. Second, we present two extensions of the Bland-Jensen equations to slightly larger systems of non-linear polynomial equations. Our systems of polynomial equations have a solution if and only if the associated matroid M is orientable. The systems come in two versions, one directly extending the Bland-Jensen system for F2, and a different system working over other fields. We study some basic algebraic properties of these systems. Finally, we present an infinite family of non-weakly-orientable matroids, with growing rank and co-rank. -
Projective Planes
Projective Planes A projective plane is an incidence system of points and lines satisfying the following axioms: (P1) Any two distinct points are joined by exactly one line. (P2) Any two distinct lines meet in exactly one point. (P3) There exists a quadrangle: four points of which no three are collinear. In class we will exhibit a projective plane with 57 points and 57 lines: the game of The Fano Plane (of order 2): SpotIt®. (Actually the game is sold with 7 points, 7 lines only 55 lines; for the purposes of this 3 points on each line class I have added the two missing lines.) 3 lines through each point The smallest projective plane, often called the Fano plane, has seven points and seven lines, as shown on the right. The Projective Plane of order 3: 13 points, 13 lines The second smallest 4 points on each line projective plane, 4 lines through each point having thirteen points 0, 1, 2, …, 12 and thirteen lines A, B, C, …, M is shown on the left. These two planes are coordinatized by the fields of order 2 and 3 respectively; this accounts for the term ‘order’ which we shall define shortly. Given any field 퐹, the classical projective plane over 퐹 is constructed from a 3-dimensional vector space 퐹3 = {(푥, 푦, 푧) ∶ 푥, 푦, 푧 ∈ 퐹} as follows: ‘Points’ are one-dimensional subspaces 〈(푥, 푦, 푧)〉. Here (푥, 푦, 푧) ∈ 퐹3 is any nonzero vector; it spans a one-dimensional subspace 〈(푥, 푦, 푧)〉 = {휆(푥, 푦, 푧) ∶ 휆 ∈ 퐹}. -
Chapter 30 Latin Square and Related Designs
Chapter 30 Latin Square and Related Designs We look at latin square and related designs. 30.1 Basic Elements Exercise 30.1 (Basic Elements) 1. Di®erent arrangements of same data. Nine patients are subjected to three di®erent drugs (A, B, C). Two blocks, each with three levels, are used: age (1: below 25, 2: 25 to 35, 3: above 35) and health (1: poor, 2: fair, 3: good). The following two arrangements of drug responses for age/health/drugs, health, i: 1 2 3 age, j: 1 2 3 1 2 3 1 2 3 drugs, k = 1 (A): 69 92 44 k = 2 (B): 80 47 65 k = 3 (C): 40 91 63 health # age! j = 1 j = 2 j = 3 i = 1 69 (A) 80 (B) 40 (C) i = 2 91 (C) 92 (A) 47 (B) i = 3 65 (B) 63 (C) 44 (A) are (choose one) the same / di®erent data sets. This is a latin square design and is an example of an incomplete block design. Health and age are two blocks for the treatment, drug. 2. How is a latin square created? True / False Drug treatment A not only appears in all three columns (age block) and in all three rows (health block) but also only appears once in every row and column. This is also true of the other two treatments (B, C). 261 262 Chapter 30. Latin Square and Related Designs (ATTENDANCE 12) 3. Other latin squares. Which are latin squares? Choose none, one or more. (a) latin square candidate 1 health # age! j = 1 j = 2 j = 3 i = 1 69 (A) 80 (B) 40 (C) i = 2 91 (B) 92 (C) 47 (A) i = 3 65 (C) 63 (A) 44 (B) (b) latin square candidate 2 health # age! j = 1 j = 2 j = 3 i = 1 69 (A) 80 (C) 40 (B) i = 2 91 (B) 92 (A) 47 (C) i = 3 65 (C) 63 (B) 44 (A) (c) latin square candidate 3 health # age! j = 1 j = 2 j = 3 i = 1 69 (B) 80 (A) 40 (C) i = 2 91 (C) 92 (B) 47 (B) i = 3 65 (A) 63 (C) 44 (A) In fact, there are twelve (12) latin squares when r = 3. -
The Structure of Binary Matroids with No Induced Claw Or Fano Plane Restriction
ADVANCES IN COMBINATORICS, 2019:1, 17 pp. www.advancesincombinatorics.com The Structure of Binary Matroids with no Induced Claw or Fano Plane Restriction Marthe Bonamy František Kardoš Tom Kelly Peter Nelson Luke Postle Received 11 June 2018; Published 30 October 2019 Abstract: An induced restriction of a simple binary matroid M is a restriction MjF, where F is a flat of M. We consider the class M of all simple binary matroids M containing neither a free matroid on three elements (which we call a claw), nor a Fano plane as an induced restriction. We give an exact structure theorem for this class; two of its consequences are that the matroids in M have unbounded critical number, while the matroids in M not containing the clique M(K5) as an induced restriction have critical number at most 2. Key words and phrases: matroid, induced. 1 Introduction This paper considers questions from the theory of induced subgraphs in the setting of simple binary matroids. We adopt a nonstandard formalism of binary matroids, incorporating the notion of an ‘ambient arXiv:1806.04188v4 [math.CO] 13 Nov 2019 space’ into the definition of a matroid itself. A simple binary matroid (hereafter just a matroid) is a pair M = (E;G), where G is a finite-dimensional binary projective geometry and the ground set E is a subset of (the points of) G. The dimension of M is the dimension of G. If E = G, then we refer to M itself as a projective geometry. If no proper subgeometry of G contains E, then M is full-rank. -
Matroid Representation, Geometry and Matrices
MATROID REPRESENTATION, GEOMETRY AND MATRICES GARY GORDON 1. Introduction The connections between algebra and finite geometry are very old, with theorems about configurations of points dating to ancient Greece. In these notes, we will put a matroid theoretic spin on these results, with matroid representations playing the central role. Recall the definition of a matroid via independent sets I. Definition 1.1. Let E be a finite set and let I be a family of subsets of E. Then the family I forms the independent sets of a matroid M if: (I1) I 6= ; (I2) If J 2 I and I ⊆ J, then I 2 I (I3) If I;J 2 I with jIj < jJj; then there is some element x 2 J − I with I [ fxg 2 I We begin with an example to show how a finite collection of vectors can be used to create a picture of the matroid. Example 1.2. Let N be the following 3 × 5 matrix: a b c d e 2 0 0 0 1 1 3 N = 4 0 1 1 0 0 5 1 1 0 1 0 Our immediate goal is to produce a configuration that represents the linear depen- dences of the columns of N. We use the following procedure: • Each column vector will be represented by a point; • If three vectors u; v and w are linearly dependent, then the corresponding three points will be collinear. Notice that columns a; b and c are linearly dependent. That means the corre- sponding three points will be collinear. This process shows that the matroid M corresponding to the matrix N is what we have depicted in Fig.