In mathematics, a closure operator on a set S is a function from the power set of S to itself that satisfies the following conditions for all sets
| (cl is extensive), | |
| (cl is increasing), | |
| (cl is idempotent). |
Closure operators are determined by their closed sets, i.e., by the sets of the form cl( X), since the closure cl( X) of a set X is the smallest closed set containing X. Such families of "closed sets" are sometimes called closure systems or " Moore families". A set together with a closure operator on it is sometimes called a closure space. Closure operators are also called " hull operators", which prevents confusion with the "closure operators" studied in topology.
There is a simple and fast algorithm for generating all closed sets of a given closure operator.Ganter, Algorithm 1
A closure operator on a set is topological if and only if the set of closed sets is closed under finite unions, i.e., C is a meet-complete sublattice of P( S). Even for non-topological closure operators, C can be seen as having the structure of a lattice. (The join of two sets X, Y ⊆ P( S) being cl( X Y).) But then C is not a sublattice of the lattice P( S).
Given a finitary closure operator on a set, the closures of finite sets are exactly the of the set C of closed sets. It follows that C is an algebraic poset. Since C is also a lattice, it is often referred to as an algebraic lattice in this context. Conversely, if C is an algebraic poset, then the closure operator is finitary.
The relative interior is not a closure operator: although it is idempotent, it is not increasing and if is a cube in and is one of its faces, then , but and , so it is not increasing.
In topology, the closure operators are topological closure operators, which must satisfy
for all (Note that for this gives ).
In algebra and logic, many closure operators are finitary closure operators, i.e. they satisfy
In the theory of partially ordered sets, which are important in theoretical computer science, closure operators have a more general definition that replaces with . (See .)
Perhaps the best known example for this is the function that associates to every subset of a given vector space its linear span. Similarly, the function that associates to every subset of a given group the subgroup generated by it, and similarly for fields and all other types of algebraic structures.
The linear span in a vector space and the similar algebraic closure in a field both satisfy the exchange property: If x is in the closure of the union of A and { y} but not in the closure of A, then y is in the closure of the union of A and { x}. A finitary closure operator with this property is called a matroid. The dimension of a vector space, or the transcendence degree of a field (over its prime field) is exactly the rank of the corresponding matroid.
The function that maps every subset of a given field to its algebraic closure is also a finitary closure operator, and in general it is different from the operator mentioned before. Finitary closure operators that generalize these two operators are studied in model theory as dcl (for definable closure) and acl (for algebraic closure).
The convex hull in n-dimensional Euclidean space is another example of a finitary closure operator. It satisfies the anti-exchange property: If x is in the closure of the union of { y} and A, but not in the union of { y} and closure of A, then y is not in the closure of the union of { x} and A. Finitary closure operators with this property give rise to .
As another example of a closure operator used in algebra, if some algebra has universe A and X is a set of pairs of A, then the operator assigning to X the smallest congruence containing X is a finitary closure operator on A x A.Clifford Bergman, Universal Algebra, 2012, Section 2.4.
This continuity condition is on the basis of a fixed point theorem for J. Consider the one-step operator J of a monotone logic. This is the operator associating any set X of formulas with the set J( X) of formulas that are either logical axioms or are obtained by an inference rule from formulas in X or are in X. Then such an operator is continuous and we can define cl( X) as the least fixed point for J greater or equal to X. In accordance with such a point of view, Tarski, Brown, Suszko and other authors proposed a general approach to logic based on closure operator theory. Also, such an idea is proposed in programming logic (see Lloyd 1987) and in fuzzy logic (see Gerla 2000).
A function cl: P → P from a partial order P to itself is called a closure operator if it satisfies the following axioms for all elements x, y in P.
| x ≤ cl( x) | (cl is extensive) |
| x ≤ y implies cl( x) ≤ cl( y) | (cl is increasing) |
| cl(cl( x)) = cl( x) | (cl is idempotent) |
More succinct alternatives are available: the definition above is equivalent to the single axiom
for all x, y in P.
Using the pointwise order on functions between posets, one may alternatively write the extensiveness property as id P ≤ cl, where id is the identity function. A self-map k that is increasing and idempotent, but satisfies the dual of the extensiveness property, i.e. k ≤ id P is called a kernel operator,Giertz, p. 26 interior operator,Erné, p. 2, uses closure (resp. interior) operation or dual closure.Blyth, p. 10 As examples, if A is a subset of a set B, then the self-map on the powerset of B given by μA( X) = A ∪ X is a closure operator, whereas λA( X) = A ∩ X is a kernel operator. The ceiling function from the to the real numbers, which assigns to every real x the smallest integer not smaller than x, is another example of a closure operator.
A fixpoint of the function cl, i.e. an element c of P that satisfies cl( c) = c, is called a closed element. A closure operator on a partially ordered set is determined by its closed elements. If c is a closed element, then x ≤ c and cl( x) ≤ c are equivalent conditions.
Every Galois connection (or residuated mapping) gives rise to a closure operator (as is explained in that article). In fact, every closure operator arises in this way from a suitable Galois connection.Blyth, p. 10 The Galois connection is not uniquely determined by the closure operator. One Galois connection that gives rise to the closure operator cl can be described as follows: if A is the set of closed elements with respect to cl, then cl: P → A is the lower adjoint of a Galois connection between P and A, with the upper adjoint being the embedding of A into P. Furthermore, every lower adjoint of an embedding of some subset into P is a closure operator. "Closure operators are lower adjoints of embeddings." Note however that not every embedding has a lower adjoint.
Any partially ordered set P can be viewed as a category theory, with a single morphism from x to y if and only if x ≤ y. The closure operators on the partially ordered set P are then nothing but the monads on the category P. Equivalently, a closure operator can be viewed as an endofunctor on the category of partially ordered sets that has the additional idempotent and extensive properties.
If P is a complete lattice, then a subset A of P is the set of closed elements for some closure operator on P if and only if A is a Moore family on P, i.e. the largest element of P is in A, and the infimum (meet) of any non-empty subset of A is again in A. Any such set A is itself a complete lattice with the order inherited from P (but the supremum (join) operation might differ from that of P). When P is the powerset Boolean algebra of a set X, then a Moore family on P is called a closure system on X.
The closure operators on P form themselves a complete lattice; the order on closure operators is defined by cl1 ≤ cl2 iff cl1( x) ≤ cl2( x) for all x in P.
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