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There is a precise correspondence between matroids and Alfred North Whitehead’s theory of dimension, as found in Mathematical Concepts of the Material World (MW), published in 1906. In brief, if (E,φ) is a geometrical system in the sense of Whitehead, where E is finite and φ-maximal, then E is a simple matroid. Within the context of Whitehead’s geometrical axioms, φ-maximal is Whitehead’s term for a simple matroid. Conversely, every simple matroid is a φ-maximal geometrical system in the sense of Whitehead.
Whitehead’s notation will be used for his theory, and Oxley’s notation will be used for matroids.
Hassler Whitney introduced matroids in 1935. I am not aware of any direct influence of Whitehead on Whitney. However, there are some significant indirect connections, as mathematicians in the same intellectual milieu. Both of them were at Harvard: Whitney as a young PhD (received in 1932), and Whitehead from 1924 until his retirement in 1937. Whitney’s PhD advisor was George Birkhoff, who had numerous interactions with Whitehead at Harvard. In fact, the Whiteheads lived two floors above the Birkhoffs on Memorial Drive, and they “were very congenial with them.” Harvard’s Society of Fellows grew out of a conversation between Whitehead and the biochemist L. J. Henderson (who, years earlier, had helped to recruit Whitehead to Harvard). When the Society was organized in 1933, George Birkhoff’s son Garrett became one of the inaugural Junior Fellows, and Whitehead became an inaugural Senior Fellow. Garrett Birkhoff was an early contributor to matroid theory, publishing the same year as Whitney in 1935. Incidently, another of the five inaugural Junior Fellows was Quine, who received his PhD under Whitehead at Harvard in 1932. The Society of Fellows met for dinner Monday nights.
Matroid theory was originally conceived as a common generalization of the notion of linear independence in vector spaces and circuits in graphs. The definition of a matroid can be presented in several ways – in terms of flats, a closure operator, a rank function, or independent sets. All of the definitions turn out to be equivalent, and the equivalence of these definitions (among others such as circuits) is the starting point of matroid theory.
Whitehead’s MW has an analogue of each of these fundamental concepts of matroid theory. His name for flats and closure was the φ-common region; his name for rank was the φ-dimension number; and his name for independent set was φ-axial. Within the context of his geometrical axioms, a φ-maximal set was his name for simple matroid. A significant part of MW is devoted to proving propositions about these concepts and their relationships.
The analogy between matroids and Whitehead’s theory is shown in the following table.
Matroid Whitehead closure operator φ-common region equal closure φ-equivalent rank φ-dimension number independent set φ-axial simple matroid φ-maximalWhitehead’s theory includes examples that lie outside the scope of matroid theory. Yet numerous propositions in MW have exact counterparts in matroid theory. The two theorems below give the precise relationship between matroids and Whitehead’s theory. The first theorem states that every finite φ-maximal geometrical system in the sense of Whitehead is a simple matroid. The second theorem states conversely that every simple matroid is a finite φ-maximal geometrical system in the sense of Whitehead.
[Whitehead’s geometrical axioms] Let E be a set, and let some of the subsets of E be designated as φ-classes. We say that (E,φ) is geometrical (or a geometrical system) in the sense of Whitehead if the following five axioms hold.
- (λ) E is a φ-class.
- (μ) For all elements x of E, the singleton {x} is a φ-class.
- (ν’) The φ-dimension number of E is finite, and the φ-common region of the empty set is the empty set.
- (π) For all subsets u of E and for all φ-axial subsets v of its φ-common region, there exists a subset w of E such that the union v∪ w is φ-axial and φ-equivalent to u.
- (ρ) For all φ-axial subsets u,v of E, if the cardinality of the union u∩ v is at least 2, then the union u∪ v is φ-maximal.
Whitehead defines φ to be geometrical if it satisfies five axioms (λ,μ,ν,π,ρ).Hp.φ. The axioms λ, μ, π and ρ are Whitehead’s axioms λ.Hp.φ, μ.Hp.φ, π.Hp.φ, and ρ.Hp.φ.
Whitehead’s axiom ν.Hp.φ is that E is three-dimensional. He makes this assumption because his interest is three-dimensional geometry, while observing that “the reasoning can be applied to higher dimensions, only more elaborate inductions and an extra axiom are required.” Whitehead does not spell out this extra axiom. We have replaced his axiom with finite-dimensionality (ν’).
Theorem. Let (E,φ) be geometrical in the sense of Whitehead. If E is finite and φ-maximal, then E is a simple matroid whose closure operator is the φ-common region operator. Moreover, a subset of E is a flat of the matroid iff it is an intersection of φ-classes. The independent sets of the matroid are the φ-axial sets (together with the empty set). Finally, the rank function on the matroid is equal to the φ-dimension number on every nonempty set.
Theorem. Let (E,I) be a simple matroid, with finite ground set E and independent sets I. Define the φ-classes to be the flats (i.e. closed sets) of the matroid. Then
- For any subset u of the ground set E, the φ-common region of u is the matroid closure of u.
- Two subsets u,v of the ground set E are φ-equivalent iff they have the same matroid closure.
- A nonempty subset of the ground set E is φ-prime iff it is an independent set of the matroid.
- The φ-dimension number of a nonempty subset of the ground set E is its matroid rank.
- If E is nonempty, then E is φ-maximal. Moreover, every φ-prime set is φ-axial.
- (E,φ) is geometrical in the sense of Whitehead.
The following pdf gives the proofs of these theorems.
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