In mathematics, in the area of order theory, a free lattice is the free object corresponding to a lattice. As free objects, they have the universal property.
Because the concept of a lattice can be axiomatised in terms of two operations and satisfying certain identities, the category of all lattices constitute a variety (universal algebra), and thus there exist (by general principles of universal algebra) free objects within this category: lattices where only those relations hold which follow from the general axioms.
These free lattices may be characterised using the relevant universal property. Concretely, free lattice is a functor from sets to lattices, assigning to each set the free lattice equipped with a set map assigning to each the corresponding element . The universal property of these is that there for any map from to some arbitrary lattice exists a unique lattice homomorphism satisfying , or as a commutative diagram: The functor is left adjoint to the forgetful functor from lattices to their underlying sets.
It is frequently possible to prove things about the free lattice directly using the universal property, but such arguments tend to be rather abstract, so a concrete construction provides a valuable alternative presentation.
In the case of semilattices, an explicit construction of the free semilattice is straightforward to give; this helps illustrate several features of the definition by way of universal property. Concretely, the free semilattice may be realised as the set of all finite nonempty subsets of , with ordinary set union as the join operation . The map maps elements of to singleton sets, i.e., for all . For any semilattice and any set map , the corresponding universal morphism is given by where denotes the semilattice operation in .
This form of is forced by the universal property: any can be written as a finite union of elements on the form for some , the equality in the universal property says , and finally the homomorphism status of implies for all . Any extension of to infinite subsets of (if there even is one) need however not be uniquely determined by these conditions, so there cannot in be any elements corresponding to infinite subsets of .
It is similarly possible to define a free functor for lower semilattices, but the combination fails to produce the free lattice in several ways, because treats as just a set:
The actual structure of the free lattice is considerably more intricate than that of the free semilattice.


The word problem for free lattices has some interesting aspects. Consider the case of bounded lattices, i.e. algebraic structures with the two binary operations ∨ and ∧ and the two constants (nullary operations) 0 and 1. The set of all wellformed expressions that can be formulated using these operations on elements from a given set of generators X will be called W(X). This set of words contains many expressions that turn out to denote equal values in every lattice. For example, if a is some element of X, then a ∨ 1 = 1 and a ∧ 1 =a. The word problem for free bounded lattices is the problem of determining which of these elements of W(X) denote the same element in the free bounded lattice FX, and hence in every bounded lattice.
The word problem may be resolved as follows. A relation ≤_{~} on W(X) may be defined inductively by setting w ≤_{~} v if and only if one of the following holds:
This defines a preorder ≤_{~} on W(X), so an equivalence relation can be defined by w ~ v when w ≤_{~} v and v ≤_{~} w. One may then show that the partially ordered quotient space W(X)/~ is the free bounded lattice FX.^{[1]}^{[2]} The equivalence classes of W(X)/~ are the sets of all words w and v with w ≤_{~} v and v ≤_{~} w. Two wellformed words v and w in W(X) denote the same value in every bounded lattice if and only if w ≤_{~} v and v ≤_{~} w; the latter conditions can be effectively decided using the above inductive definition. The table shows an example computation to show that the words x∧z and x∧z∧(x∨y) denote the same value in every bounded lattice. The case of lattices that are not bounded is treated similarly, omitting rules 2. and 3. in the above construction.
The solution of the word problem on free lattices has several interesting corollaries. One is that the free lattice of a threeelement set of generators is infinite. In fact, one can even show that every free lattice on three generators contains a sublattice which is free for a set of four generators. By induction, this eventually yields a sublattice free on countably many generators.^{[3]} This property is reminiscent of SQuniversality in groups.
The proof that the free lattice in three generators is infinite proceeds by inductively defining
where x, y, and z are the three generators, and p_{0} = x. One then shows, using the inductive relations of the word problem, that p_{n+1} is strictly greater^{[4]} than p_{n}, and therefore all infinitely many words p_{n} evaluate to different values in the free lattice FX.
Another corollary is that the complete free lattice (on three or more generators) "does not exist", in the sense that it is a proper class. The proof of this follows from the word problem as well. To define a complete lattice in terms of relations, it does not suffice to use the finitary relations of meet and join; one must also have infinitary relations defining the meet and join of infinite subsets. For example, the infinitary relation corresponding to "join" may be defined as
Here, f is a map from the elements of a cardinal N to FX; the operator denotes the supremum, in that it takes the image of f to its join. This is, of course, identical to "join" when N is a finite number; the point of this definition is to define join as a relation, even when N is an infinite cardinal.
The axioms of the preordering of the word problem may be adjoined by the two infinitary operators corresponding to meet and join. After doing so, one then extends the definition of to an ordinally indexed given by
when is a limit ordinal. Then, as before, one may show that is strictly greater than . Thus, there are at least as many elements in the complete free lattice as there are ordinals, and thus, the complete free lattice cannot exist as a set, and must therefore be a proper class.