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Bounded lattice

In mathematics, and in particular in order theory, a bounded lattice is a lattice that has a least element and a greatest element, usually denoted by and , respectively.

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In mathematics, and in particular in order theory, a bounded lattice is a lattice that has a least element and a greatest element, usually denoted by 0 {\displaystyle 0} and 1 {\displaystyle 1} , respectively.1

Bounded lattices are of considerable importance because many algebraic structures are bounded lattices, including complete lattices, Heyting algebras, Boolean algebras, and others.

Definition

A bounded lattice can be defined in two equivalent ways: via an order relation or algebraically. These two definitions can be shown to be equivalent.

Order-theoretic definition

Let ( L , ) {\displaystyle (L,\leq )} be a partially ordered set. Then L {\displaystyle L} is called a bounded lattice if and only if:

  1. L {\displaystyle L} is a lattice with respect to the order relation:
    1. For every pair a , b L {\displaystyle a,b\in L} , there exists an infimum.
    2. For every pair a , b L {\displaystyle a,b\in L} , there exists a supremum.
  2. L {\displaystyle L} is a bounded poset:
    1. There exists m L {\displaystyle m\in L} such that for every a L {\displaystyle a\in L} , m a {\displaystyle m\leq a} . This element is unique and is denoted by 0 {\displaystyle 0} .
    2. There exists M L {\displaystyle M\in L} such that for every a L {\displaystyle a\in L} , a M {\displaystyle a\leq M} . This element is unique and is denoted by 1 {\displaystyle 1} .

Algebraic definition

Let L {\displaystyle L} be a set equipped with two binary operations {\displaystyle \land } and {\displaystyle \lor } , and two distinguished elements 0 , 1 L {\displaystyle 0,1\in L} . Then L {\displaystyle L} is called a bounded lattice if and only if the following conditions hold:

  1. L {\displaystyle L} is a lattice with respect to {\displaystyle \land } and {\displaystyle \lor } :
    1. Associativity: for all a , b , c L {\displaystyle a,b,c\in L} , ( a b ) c = a ( b c ) {\displaystyle (a\land b)\land c=a\land (b\land c)} and ( a b ) c = a ( b c ) {\displaystyle (a\lor b)\lor c=a\lor (b\lor c)} .
    2. Commutativity: for all a , b L {\displaystyle a,b\in L} , a b = b a {\displaystyle a\land b=b\land a} and a b = b a {\displaystyle a\lor b=b\lor a} .
    3. Idempotence: for all a L {\displaystyle a\in L} , a a = a {\displaystyle a\land a=a} and a a = a {\displaystyle a\lor a=a} .
    4. Absorption: for all a , b L {\displaystyle a,b\in L} , a ( a b ) = a {\displaystyle a\land (a\lor b)=a} and a ( a b ) = a {\displaystyle a\lor (a\land b)=a} .
  2. 0 {\displaystyle 0} and 1 {\displaystyle 1} are identity elements for {\displaystyle \lor } and {\displaystyle \land } , respectively:
    1. For all a L {\displaystyle a\in L} , a 0 = a {\displaystyle a\lor 0=a} .
    2. For all a L {\displaystyle a\in L} , a 1 = a {\displaystyle a\land 1=a} .

Properties

  • In a bounded lattice ( L , , , 0 , 1 ) {\displaystyle (L,\land ,\lor ,0,1)} , for every a L {\displaystyle a\in L} , one has a 0 = 0 {\displaystyle a\land 0=0} .
  • In a bounded lattice ( L , , , 0 , 1 ) {\displaystyle (L,\land ,\lor ,0,1)} , for every a L {\displaystyle a\in L} , one has a 1 = 1 {\displaystyle a\lor 1=1} .

Bounding a lattice

Let ( L , ) {\displaystyle (L,\leq )} be an arbitrary lattice. One may ask whether there exists a bounded lattice L {\displaystyle L'} into which L {\displaystyle L} can be order-embedded.

Define L := { x x L } { , L } {\displaystyle L':=\{\downarrow \!x\mid x\in L\}\cup \{\emptyset ,L\}} , a collection of subsets of L {\displaystyle L} , where for each x L {\displaystyle x\in L} , x {\displaystyle \downarrow \!x} denotes the principal lower set generated by x {\displaystyle x} . It can be shown that L {\displaystyle L'} , ordered by inclusion {\displaystyle \subseteq } , is a bounded lattice. Define a function φ : L L {\displaystyle \varphi \colon L\to L'} by φ ( x ) :=↓ x {\displaystyle \varphi (x):=\downarrow \!x} . One can prove that φ {\displaystyle \varphi } is an order embedding.

The Dedekind–MacNeille completion proves a much stronger statement: every partially ordered set (not necessarily a lattice) can be embedded into a complete lattice (which is necessarily bounded).2

Complemented lattice

Let ( L , , , 0 , 1 ) {\displaystyle (L,\land ,\lor ,0,1)} be a bounded lattice. It is called a complemented lattice if and only if for every a L {\displaystyle a\in L} there exists b L {\displaystyle b\in L} such that a b = 0 {\displaystyle a\land b=0} and a b = 1 {\displaystyle a\lor b=1} .

In this case, b {\displaystyle b} is called a complement of a {\displaystyle a} . In contrast to a Boolean algebra, a complemented lattice may have more than one complement for a given element. Intuitively, a complement can be thought of as a negation of the element.

Examples

  • Every finite partially ordered set that is a lattice is a complete lattice, and hence a bounded lattice.
  • Let L {\displaystyle L} be the collection of all vector subspaces of R 2 {\displaystyle \mathbb {R} ^{2}} , ordered by inclusion. This is a bounded lattice with minimum 0 {\displaystyle {0}} and maximum R 2 {\displaystyle \mathbb {R} ^{2}} .
  • Let C {\displaystyle C} be the set of all continuous functions from R {\displaystyle \mathbb {R} } to the closed interval [ 0 , 1 ] {\displaystyle [0,1]} , ordered pointwise: f g {\displaystyle f\leq g} if and only if f ( x ) g ( x ) {\displaystyle f(x)\leq g(x)} for all x R {\displaystyle x\in \mathbb {R} } . Then ( C , ) {\displaystyle (C,\leq )} is a lattice, since for any two functions one may take their pointwise minimum and maximum, which are again continuous. However, for an infinite family of continuous functions, this construction need not yield a continuous function. Hence, this lattice is not complete. It is bounded, since the constant functions m ( x ) := 0 {\displaystyle m(x):=0} and M ( x ) := 1 {\displaystyle M(x):=1} serve as global minimum and maximum.
  • Let P {\displaystyle P} be the collection of all convex and closed polygons in R 2 {\displaystyle \mathbb {R} ^{2}} , together with the empty set {\displaystyle \emptyset } and the whole space R 2 {\displaystyle \mathbb {R} ^{2}} , ordered by inclusion. This is a lattice because the intersection of two closed convex polygons is again a closed convex polygon, and the closure of the convex hull of their union is also a closed convex polygon. It is bounded, with {\displaystyle \emptyset } as minimum and R 2 {\displaystyle \mathbb {R} ^{2}} as maximum. However, it is not complete: the family of all closed convex polygons contained in the unit disk has no supremum in this lattice, since their union is a circle, which is not a polygon.
References

References

  1. Grätzer, George (2011). Lattice Theory: Foundation. doi:10.1007/978-3-0348-0018-1.
  2. Schröder, Bernd (2016). Ordered Sets. doi:10.1007/978-3-319-29788-0.