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This book is the second in a three-volume series, the first of which is Theory of Matroids, and the third of which will be called Combinatorial Geometries: Advanced Theory. The three volumes together will constitute a fairly complete survey of the current knowledge of matroids and their closely related cousins, combinatorial geometries. As in the first volume, clear exposition of our subject has been one of our main goals, so that the series will be useful not only as a reference for specialists, but also as a textbook for graduate students and a first introduction to the subject for all who are interested in using matroid theory in their work.
This volume begins with three chapters on coordinatization or vector representation, by Fournier and White. They include a general chapter on ‘Coordinatizations,’ and two chapters on the important special cases of ‘Binary Matroids’ and ‘Unimodular Matroids’ (also known as regular matroids). These are followed by two chapters by Brualdi, titled ‘Introduction to Matching Theory’ and ‘Transversal Matroids,’ and a chapter on ‘Simplicial Matroids’ by Cordovil and Lindstrom. These six chapters, together with Oxley's ‘Graphs and Series-Parallel Networks’ from the first volume, constitute a survey of the major special types of matroids, namely, graphic matroids, vector matroids, transversal matroids, and simplicial matroids. We follow with two chapters on the important matroids invariants, ‘The Mobius Function and the Characteristic Polynomial’ by Zaslavsky and ‘Whitney Numbers’ by Aigner. We conclude with a chapter on the aspect of matroid theory that is primarily responsible for an explosion of interest in the subject in recent years, ‘Matroids in Combinatorial Optimization’ by Faigle.
Binary matroids play an important theoretical role, partly because they were the first class of coordinatizable matroids to be completely characterized, but also because the class of binary matroids contains the unimodular matroids and the graphic matroids, two classes fundamental to matroid theory. There are numerous characterizations of binary matroids, very different in nature, and expressive of the richness of the concept.
Definition and Basic Properties
Definition. A matroid is binary if it is representable (coordinatizable) over the two-element field GF(2).
According to the general definition of representable matroids, (see Chapter 1), a matroid M(E) on a finite set E is binary if there is a mapping α of E into a GF(2)-vector space V such that a subset X ⊆ E is independent in M(E) if and only if the restriction of α to X is injective and the set {α(x)|x ∈ X} of vectors in V is linearly independent. The mapping a is then called a binary representation of the matroid M(E).
Example. Denote by Ur,n up to isomorphism, the matroid on a set of n elements, in which the bases are those subsets which have r elements. Then U2,3 is binary. (This matroid is identified with the projective line over the field GF(2).) On the other hand, U2,4. is not binary; this matroid, which consists of four geometric points on a line, is a typical non-binary matroid, and serves to characterize the binary matroids, as we shall see later.
Matroids enter combinatorial optimization problems at various levels. Whitney's (1935) motivation to introduce matroids as combinatorial objects in their own right stemmed from his interest in approaching the Four-Color Problem algebraically and combining the combinatorial and algebraic-geometric aspects of graphs into the notion of a matroid.
Graphs furnish the most important models for combinatorial optimization problems. Thus it is natural to ask to what extent graph properties actually are properties of the underlying matroid and to study more general classes of matroids that enjoy, for example, the ‘max-flow-min-cut’ property of network flows (cf. Seymour 1977). This approach leads to fundamental structural questions about matroids per se which, nevertheless, have many practical implications. One of the foremost results in this area is Seymour's (1980) decomposition theory for regular matroids exhibiting regular matroids as being essentially built up by graphic and cographic matroids. As a consequence, efficient procedures can be developed to test whether a matrix is totally unimodular or whether certain linear programs actually are (better tractable) network problems (see, e.g., Welsh 1982 and Bixby 1982 for an introduction into this aspect of matroid theory).
Matroids also compose the combinatorial structure of linear programming (Minty 1966, Rockafellar 1969). Indeed, pivoting in linear programming may be carried out purely ‘combinatorially’ (Bland 1977).
The purpose of this chapter is to provide background and general results concerning coordinatizations, while the more specialized subtopics of binary and unimodular matroids are covered in later chapters. The first section of this chapter is devoted to definitions and notational conventions. The second section concerns linear and projective equivalence of coordinatizations. Although they are not usually explicitly considered in other expositions of matroid coordinatization, these equivalence relations are very useful in working with examples of coordinatizations, as well as theoretically useful as in Proposition 1.2.5. Section 1.3 involves the preservation of coordinatizability under certain standard matroid operations, including duality and minors. The next section presents some well-known counterexamples, and Section 1.5 considers characterizations of coordinatizability, especially characterizations by excluded minors. The final five sections are somewhat more technical in nature, and may be omitted by the reader who desires only an introductory survey. Section 1.6 concerns the bracket conditions, another general characterization of coordinatizability. Section 1.7 presents techniques for construction of a matroid requiring a root of any prescribed polynomial in a field over which we wish to coordinatize it. These techniques are extremely useful in the construction of examples and counterexamples, yet are not readily available in other works, except Greene (1971). The last three sections concern characteristic sets, the use of transcendentals in coordinatizations, and algebraic representation (i.e., modeling matroid dependence by algebraic dependence). Some additional topics which could have been considered here, such as chain groups, are omitted because they are well-covered in other readily available sources, such as Welsh (1976).
A large body of mathematics consists of facts that can be presented and described much like any other natural phenomenon. These facts, at times explicitly brought out as theorems, at other times concealed within a proof, make up most of the applications of mathematics, and are the most likely to survive change of style and of interest.
This ENCYCLOPEDIA will attempt to present the factual body of all mathematics. Clarity of exposition, accessibility to the nonspecialist, and a thorough bibliography are required of each author. Volumes will appear in no particular order, but will be organized into sections, each one comprising a recognizable branch of present-day mathematics. Numbers of volumes and sections will be reconsidered as times and needs change.
It is hoped that this enterprise will make mathematics more widely used where it is needed, and more accessible in fields in which it can be applied but where it has not yet penetrated because of insufficient information.
For α≥0 and β≥0 we denote by K (α, β) the Kaplan classes of functions f analytic and non-zero in the open unit disk U = {z: |z| < 1} such that f ∈ K(α, β), if, and only if, for θ1 < θ2 < θ1 + 2π and 0 < r < 1,
Consider an impermeable container Ω in ℝ3 filled with a porous material saturated with a Boussinesq fluid. The boundary ∂Ω of Ω consists of two parts Γ1 and Γ2, i. e., ∂Ω = Γ1 ⋃ Γ2. Γ1 is the intersection of the horizontal planes at z = 0 and z = 1 with a vertical cylinder of arbitrary cross section G (a bounded smooth domain in ℝ2), i.e., Γ1 = G × {0, 1}. Γ2 is the sidewall of the vertical cylinder between the planes z = 0 and z = l, i.e., Γ2Γ = ∂G × [0, 1].