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Kuratowski closure axioms

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In topology and related branches of mathematics, the Kuratowski closure axioms are a set of axioms that can be used to define a topological structure on a set. They are equivalent to the more commonly used open set definition. They were first formalized by Kazimierz Kuratowski,[1] although the idea had been circulating for some decades among mathematicians such as Wacław Sierpiński and António Monteiro.[2]

A similar set of axioms can be used to define a topological structure using only the dual notion of interior operator.

Definition

Kuratowski closure operators and weakenings

Let be an arbitrary set and its power set. A Kuratowski closure operator is a unary operation with the following properties:

[K1] It preserves the empty set: ;

[K2] It is extensive: for all , ;

[K3] It is idempotent: for all , ;

[K4] It preserves binary unions: for all , .

Because of extensivity [K2], it is possible to weaken the equality in [K3] to a simple inclusion. Furthermore, a consequence of preserving binary unions is the stronger condition:[3]

[K4'] It is isotonic: .

It is straightforward to show that weakening the equality in [K4] to a simple inclusion (subadditivity) and assuming [K4'] yields back to [K4] (see the next-to-last paragraph of Proof 2 below).

Kuratowski (1966) includes a fifth (optional) axiom requiring that singleton sets should be stable under closure: for all , . He refers to topological spaces which satisfy all five axioms as T1-spaces in contrast to the more general spaces which only satisfy the four listed axioms. Indeed, these spaces correspond exactly to the topological T1-spaces via the usual correspondence (see below).[1]

If requirement [K3] is omitted, then the axioms define a Čech closure operator.[4] If [K1] is omitted instead, then an operator satisfying [K2], [K3] and [K4'] is said to be a Moore closure operator.[5] A pair is called Kuratowski, Čech or Moore closure space depending on the axioms satisfied by .

Alternative axiomatizations

The four Kuratowski closure axioms can be replaced by a single condition, given by Pervin:[6]

[P] For all , .

Axioms [K1][K4] can be derived as a consequence of this requirement:

  1. Choose . Then , or . This immediately implies [K1].
  2. Choose an arbitrary and . Then, applying axiom [K1], , implying [K2].
  3. Choose and an arbitrary . Then, applying axiom [K1], , which is [K3].
  4. Choose arbitrary . Applying axioms [K1][K3], one derives [K4].

Alternatively, A. Monteiro had proposed a weaker axiom that only entails [K2][K4]:[7]

[M] For all , .

Requirement [K1] is independent of [M] : indeed, if , the operator defined by the constant assignment satisfies [M] but does not preserve the empty set, since . Notice that, by definition, any operator satisfying [M] is a Moore closure operator.

A more symmetric alternative to [M] was also proven by M. O. Botelho and M. H. Teixeira to imply axioms [K2][K4]:[2]

[BT] For all , .

Interior, exterior and boundary operators

A dual notion to Kuratowski closure operators is that of Kuratowski interior operator, which is a map satisfying the following similar requirements:[8]

[I1] It preserves the total space: ;

[I2] It is intensive: for all , ;

[I3] It is idempotent: for all , ;

[I4] It preserves binary intersections: for all , .

For these operators, one can reach conclusions that are completely analogous to what was inferred for Kuratowski closures. For example, all Kuratowski interior operators are isotonic, i.e. they satisfy [K4'], and because of intensivity [I2], it is possible to weaken the equality in [I3] to a simple inclusion.

The duality between Kuratowski closures and interiors is provided by the natural complement operator on , the map sending . This map is an orthocomplementation on the power set lattice, meaning it satisfies De Morgan's laws: if is an arbitrary set of indices and ,By employing these laws, together with the defining properties of , one can show that any Kuratowski interior induces a Kuratowski closure (and vice-versa), via the defining relation (and ). Pervin (1964) further provides analogous axioms for Kuratowski exterior operators[8] and Kuratowski boundary operators[9], which also induce Kuratowski closures via the relations and .

Abstract operators

Notice that axioms [K1][K4] may be adapted to define an abstract unary operation on a general bounded lattice , by formally substituting set-theoretic inclusion with the partial order associated to the lattice, set-theoretic union with the join operation, and set-theoretic intersections with the meet operation; similarly for axioms [I1][I4]. If the lattice is orthocomplemented, these two abstract operations induce one another in the usual way. Abstract closure or interior operators can be used to define a generalized topology on the lattice.

Since neither unions nor the empty set appear in the requirement for a Moore closure operator, the definition may be adapted to define an abstract unary operator on an arbitrary poset .

Connection to other axiomatizations of topology

Induction of topology from closure

A closure operator naturally induces a topology as follows. Let be an arbitrary set. We shall say that a subset is closed with respect to a Kuratowski closure operator if and only if it is a fixed point of said operator, or in other words it is stable under , i.e. . The claim is that the family of all subsets of the total space that are complements of closed sets satisfies the three usual requirements for a topology, or equivalently, the family of all closed sets satisfies the following:

[T1] It is a bounded sublattice of , i.e. ;

[T2] It is complete under arbitrary intersections, i.e. if is an arbitrary set of indices and , then ;

[T3] It is complete under finite unions, i.e. if is a finite set of indices and , then .

Notice that, by extensivity [K2], one may succintly write , where .

Proof 1.

[T1] By extensivity [K2], and since closure maps the power set of into itself (that is, the image of any subset is a subset of ), we have . Thus . The preservation of the empty set [K1] readily implies .

[T2] Next, let be an arbitrary set of indices and closed for every . By extensivity [K2], . Also, by isotonicity [K4'], if for all indices , then for all , which implies . Therefore, , meaning .

[T3] Finally, let be a finite set of indices and let be closed for every . From the preservation of binary unions [K4], and using induction on the number of subsets of which we take the union, we have . Thus, .

Since idempotency [K3] is not employed in the proof, this result also holds when is a Čech closure operator.[10]

Induction of closure from topology

Conversely, given a family satisfying axioms [T1][T3], it is possible to construct a Kuratowski closure operator in the following way: if and is the inclusion upset of , then defines a Kuratowski closure operator on .

Proof 2.

[K1] Since , reduces to the intersection of all sets in the family ; but by axiom [T1], so the intersection collapses to the null set and [K1] follows.

[K2] By definition of , we have that for all , and thus must be contained in the intersection of all such sets. Hence follows extensivity [K2].

[K3] Notice that, for all , the family contains itself as a minimal element w.r.t. inclusion. Hence , which is idempotence [K3].

[K4’] Let : then , and thus . Since the latter family may contain more elements than the former, we find , which is isotonicity [K4']. Notice that isotonicity implies and , which together imply .

[K4] Finally, fix . Axiom [T2] implies ; furthermore, axiom [T2] implies that . By extensivity [K2] one has and , so that . But , so that all in all . Since then is a minimal element of w.r.t. inclusion, we find . Point 4. ensures additivity [K4].

Hereditary closure

In any induced topology (relative to the subset A) the closed sets induce a new closure operator that is just the original closure operator restricted to A: [11]

Recovering notions from topology

Closeness
A point is close to a subset if

Continuity
A function is continuous at a point if

See also

Notes

  1. ^ a b Kuratowski (1966), p. 38.
  2. ^ a b Monteiro (1945), p. 160.
  3. ^ Pervin (1964), p. 43, Exercise 6.
  4. ^ Arkhangel'skij & Fedorchuk (1990), p. 25.
  5. ^ "Moore closure". nLab. March 7, 2015. Retrieved August 19, 2019. {{cite web}}: Cite has empty unknown parameter: |dead-url= (help)
  6. ^ Pervin (1964), p. 42, Exercise 5.
  7. ^ Monteiro (1945), p. 158.
  8. ^ a b Pervin (1964), p. 44.
  9. ^ Pervin (1964), p. 46, Exercise 4.
  10. ^ Arkhangel'skij & Fedorchuk (1990), p. 26.
  11. ^ Pervin (1964), p. 49, Theorem 3.4.3.

References