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In the mathematical discipline of order theory, and in particular, in lattice theory, a complemented lattice is a bounded lattice (that is it has a least element 0 and a greatest element 1), in which each element x has a complement, defined as an element y such that

x\wedge y=0    and     \quad x\vee y=1.

Uniqueness


In general an element x may have more than one complement. However in a distributive lattice, that is a lattice in which, for all x, y and z, the distributive law holds:

x \wedge (y \vee z) = (x \wedge y) \vee (x \wedge z),

which is also bounded, then each element x will have at most one complement.

Similarly, in an orthocomplemented lattice it can be shown that each element has exactly one complement - in fact, there is an idempotent order-reversing function from elements to their complements.

Thus in a Boolean algebra, which is both a complemented distributive lattice and an orthocomplemented lattice, complements exist and are unique.

Lattice theory

Vikipedio:Projekto matematiko/Komplementa krado | 有补格

 

This article is licensed under the GNU Free Documentation License. It uses material from the "Complemented lattice".

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