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In mathematics, a lattice is a partially ordered set in which all nonempty finite subsets have a least upper bound (also called supremum or join) and a greatest lower bound (also called infimum or meet). The term "lattice" comes from the shape of the Hasse diagrams of such orders.
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2 Homomorphisms 3 Properties of lattices, examples 4 Important lattice-theoretic notions 5 Literature |
A lattice can also be algebraically defined as a set L, together with two binary operations ∧ and ∨ (pronounced meet and join, respectively), such that for any a, b, c in L,
Algebraic definition
| a ∨ a = a | a ∧ a = a | idempotency laws |
| a ∨ b = b ∨ a | a ∧ b = b ∧ a | commutativity laws |
| a ∨ (b ∨ c) = (a ∨ b) ∨ c | a ∧ (b ∧ c) = (a ∧ b) ∧ c | associativity laws |
| a ∨ (a ∧ b) = a | a ∧ (a ∨ b) = a | absorption laws |
(The idempotency laws can be deduced from the absorption laws and therefore don't have to be stated separately.)
If the two operations satisfy these algebraic rules then they define a partial order ≤ on L by the following rule: a ≤ b if and only if a ∨ b = b, or, equivalently, a ∧ b = a. L, together with the partial order ≤ so defined, will then be a lattice in the above order-theoretic sense.
Conversely, if an order-theoretic lattice (L, ≤) is given, and we write a ∨ b for the least upper bound of {a, b} and a ∧ b for the greatest lower bound of {a, b}, then (L, ∨, ∧) satisfies all the axioms of an algebraically defined lattice.
The class of all lattices forms a category if we define a homomorphism between two lattices (L, ∧, ∨) and (N, ∩, ∪) to be a function f : L → N such that
Homomorphisms
for all a, b in L. If a homomorphism is bijective, then its inverse is also a homomorphism, and it is called an isomorphism of lattices. The two involved lattices are then isomorphic; for all practical purposes, they are identical and differ only in the notation of their elements.
Every homomorphism is a monotone map between the two lattices, but not every monotone map yields a lattice homomorphism: in addition we need the compatibility with finite suprema and infima.
A lattice is said to be bounded if it has a greatest element and a least element. The greatest element is often denoted by 1 and the least element by 0. If x is an element of a bounded lattice then any element y of the lattice satisfying x ∧ y = 0 and x ∨ y = 1 is called a complement of x. A bounded lattice in which every element has a (not necessarily unique) complement is called a complemented lattice.
A lattice in which every subset (including infinite ones) has a supremum and an infimum is called a complete lattice. (It is enough to require that every subset have a supremum; the existence of all infima then follows.) Complete lattices are always bounded. Many of the most important lattices are complete. Examples include:
Properties of lattices, examples
The Knaster-Tarski theorem states that the set of fixed points of a monotone function on a complete lattice is again a complete lattice.
The lattice of submodules of a module and the lattice of normal subgroups of a group have the special property that x ∨ (y ∧ (x ∨ z)) = (x ∨ y) ∧ (x ∨ z) for all x, y and z in the lattice. A lattice with this property is called a modular lattice. The condition of modularity can also be stated as follows: If x ≤ z then for all y we have the identity x ∨ (y ∧ z) = (x ∨ y) ∧ z.
A lattice is called distributive if ∨ distributes over ∧, that is, x ∨ (y ∧ z) = (x ∨ y) ∧ (x ∨ z). Equivalently, ∧ distributes over ∨. All distributive lattices are modular. Two important types of distributive lattices are totally ordered sets and Boolean algebras (like the lattice of all subsets of a given set). The lattice of natural numbers, ordered by divisibility, is also distributive. A lattice is said to be completely distributive if the above distributivity law hold for arbitrary (infinite) meets and joins. Distributive lattices are used to formulate pointless topology.
In the following, let L be a lattice. We define some order-theoretic notions that are of particular importance in lattice theory.
An element x of L is called join-irreducible iff
An element x of L is called join-prime iff
Other important notions in lattice theory are ideal and its dual notion filter. Both terms describe special subsets of a lattice (or of any partially ordered set in general). Details can be found in the respective articles.Important lattice-theoretic notions
When the first condition is generalized to arbitrary joins Vai, x is called completely join-irreducible.
The dual notion is called meet-irreducability. Sometimes one also uses the terms ∨-irreducible and ∧-irreducible, respectively.
Again, this can be generalized to obtain the notion completely join-prime and dualized to yield meet-prime. Any join-prime element is also join-irreducible, and any meet-prime element is also meet-irreducible. If the lattice is distributive the converse is also true.