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Pseudocomplement

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 with the property that . More formally, . 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, a pseudocomplemented lattice can be endowed with a unary operation * mapping every element to its pseudocomplement; this structure is sometimes called a p-algebra. However this latter term may have other meanings in other areas of mathematics.

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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 xL is said to have a pseudocomplement if there exists a greatest element x L {\displaystyle x^{*}\in L} with the property that x x = 0 {\displaystyle x\wedge x^{*}=0} . More formally, x = max { y L x y = 0 } {\displaystyle x^{*}=\max\{y\in L\mid x\wedge 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.12 However this latter term may have other meanings in other areas of mathematics.

Properties

In a p-algebra L, for all x , y L : {\displaystyle x,y\in L:} 12

  • The map x x {\displaystyle x\mapsto x^{*}} is antitone. In particular, 0 = 1 {\displaystyle 0^{*}=1} and 1 = 0 {\displaystyle 1^{*}=0} .
  • The map x x {\displaystyle x\mapsto x^{**}} is a closure.
  • x = x {\displaystyle x^{*}=x^{***}} .
  • ( x y ) = x y {\displaystyle (x\vee y)^{*}=x^{*}\wedge y^{*}} .
  • ( x y ) = x y {\displaystyle (x\wedge y)^{**}=x^{**}\wedge y^{**}} .
  • x ( x y ) = x y {\displaystyle x\wedge (x\wedge y)^{*}=x\wedge y^{*}} .

The set S ( L ) = d e f { x x L } {\displaystyle S(L){\stackrel {\mathrm {d} ef}{=}}\{x^{*}\mid x\in L\}} is called the skeleton of L. S(L) is a {\displaystyle \wedge } -subsemilattice of L and together with x y = ( x y ) = ( x y ) {\displaystyle x\cup y=(x\vee y)^{**}=(x^{*}\wedge y^{*})^{*}} forms a Boolean algebra (the complement in this algebra is {\displaystyle ^{*}} ).12 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 {\displaystyle x^{*}=0} (or equivalently, x = 1 {\displaystyle x^{**}=1} ) is called dense. Every element of the form x x {\displaystyle x\vee x^{*}} is dense. D(L), the set of all the dense elements in L is a filter of L.12 A distributive p-algebra is Boolean if and only if D ( L ) = { 1 } {\displaystyle 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 : {\displaystyle x,y\in L:} 1
    • S(L) is a sublattice of L;
    • ( x y ) = x y {\displaystyle (x\wedge y)^{*}=x^{*}\vee y^{*}} ;
    • ( x y ) = x y {\displaystyle (x\vee y)^{**}=x^{**}\vee y^{**}} ;
    • x x = 1 {\displaystyle x^{*}\vee 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 {\displaystyle a\wedge c\leq b} . This binary operation is denoted a b {\displaystyle a\to 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 {\displaystyle a^{*}} could be defined using relative pseudocomplement as a 0 {\displaystyle a\to 0} .4

See also

See also

References

References

  1. T.S. Blyth (2006). Lattices and Ordered Algebraic Structures. Springer Science & Business Media. Chapter 7. Pseudocomplementation; Stone and Heyting algebras. pp. 103–119. ISBN 978-1-84628-127-3.
  2. Clifford Bergman (2011). Universal Algebra: Fundamentals and Selected Topics. CRC Press. pp. 63–70. ISBN 978-1-4398-5129-6.
  3. Balbes, Raymond; Horn, Alfred (September 1970). "Stone Lattices". Duke Math. J. 37 (3): 537–545. doi:10.1215/S0012-7094-70-03768-3.
  4. Birkhoff, Garrett (1973). Lattice Theory (3rd ed.). AMS. p. 44.