Pseudocomplement

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In mathematics, particularly in order theory, a pseudocomplement is one generalization of the notion of complement. In a lattice L with bottom element 0, an element x ∈ L is said to have a pseudocomplement if there exists a greatest element x∗∈L with the property that x∧x∗=0. More formally, x∗=max⁡{y∈L∣x∧y=0}. The lattice L itself is called a pseudocomplemented lattice if every element of L is pseudocomplemented. Every pseudocomplemented lattice is necessarily bounded, i.e. it has a 1 as well. Since the pseudocomplement is unique by definition (if it exists), a pseudocomplemented lattice can be endowed with a unary operation * mapping every element to its pseudocomplement; this structure is sometimes called a p-algebra.[1][2] However this latter term may have other meanings in other areas of mathematics.

Properties

In a p-algebra L, for all x,y∈L:[1][2]

  • The map x↦x∗ is antitone. In particular, 0∗=1 and 1∗=0.
  • The map x↦x∗∗ is a closure.
  • x∗=x∗∗∗.
  • (x∨y)∗=x∗∧y∗.
  • (x∧y)∗∗=x∗∗∧y∗∗.
  • x∧(x∧y)∗=x∧y∗.

The set S(L)=def{x∗∣x∈L} is called the skeleton of L. S(L) is a ∧-subsemilattice of L and together with x∪y=(x∨y)∗∗=(x∗∧y∗)∗ forms a Boolean algebra (the complement in this algebra is ∗).[1][2] In general, S(L) is not a sublattice of L.[2] In a distributive p-algebra, S(L) is the set of complemented elements of L.[1]

Every element x with the property x∗=0 (or equivalently, x∗∗=1) is called dense. Every element of the form x∨x∗ is dense. D(L), the set of all the dense elements in L is a filter of L.[1][2] A distributive p-algebra is Boolean if and only if D(L)={1}.[1]

Pseudocomplemented lattices form a variety; indeed, so do pseudocomplemented semilattices.[3]

Examples

  • Every finite distributive lattice is pseudocomplemented.[1]
  • Every Stone algebra is pseudocomplemented. In fact, a Stone algebra can be defined as a pseudocomplemented distributive lattice L in which any of the following equivalent statements hold for all x,y∈L:[1]
    • S(L) is a sublattice of L;
    • (x∧y)∗=x∗∨y∗;
    • (x∨y)∗∗=x∗∗∨y∗∗;
    • x∗∨x∗∗=1.
  • Every Heyting algebra is pseudocomplemented.[1]
  • If X is a topological space, the (open set) topology on X is a pseudocomplemented (and distributive) lattice with the meet and join being the usual union and intersection of open sets. The pseudocomplement of an open set A is the interior of the set complement of A. Furthermore, the dense elements of this lattice are exactly the dense open subsets in the topological sense.[2]

Relative pseudocomplement

A relative pseudocomplement of a with respect to b is a maximal element c such that a∧c≤b. This binary operation is denoted a→b. A lattice with a relative pseudocomplement for each pair of elements is called an implicative lattice, or Brouwerian lattice. In general, an implicative lattice may not have a minimal element. If such a minimal element exists, then each pseudocomplement a∗ could be defined using relative pseudocomplement as a→0.[4]

See also

References

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