If E is a vector space over a field K, then any regular symmetric bilinear form ϕ on E induces a polarity M → M ⊥ on the lattice of all subspaces of E. In the particular case where E is 3-dimensional, the set of all subspaces M of E such that both M and M ⊥ are not N -subspaces (which, in most cases, is equivalent to saying that M is nonisotropic), ordered by inclusion and endowed with the restriction of the above polarity, is an orthomodular lattice T (E, ϕ). We show that if K is a proper subfield of K, with K = F 2 , and E a 3-dimensional K -subspace of E such that the restriction of ϕ to E × E is, up to multiplicative constant, a bilinear form ϕ on the K -space E , then T (E , ϕ ) is isomorphic to an irreducible 3-homogeneous proper subalgebra of T (E, ϕ). Our main result is a structure theorem stating that, when K is not of characteristic 3, the converse is true, i.e., any irreducible 3-homogeneous proper subalgebra of T (E, ϕ) is of this form. As a corollary, we construct infinitely many finite orthomodular lattices which are minimal in the sense that all their proper subalgebras are modular. In fact, this last result was our initial aim in this paper.
PreliminariesLet us recall some basic notions of the theory of orthomodular lattices (abbreviated OMLs). For more details the reader may consult [12] or [14].An OML is an algebra (L, 0, 1, ∨, ∧, ⊥ ), where (L, 0, 1, ∨, ∧) is a bounded lattice, and ⊥ is an antitone (i.e., such that a ≤ b implies b ⊥ ≤ a ⊥ ) and involutive unary operation so that a ∨ a ⊥ = 1 (which implies a ∧ a ⊥ = 0), and the orthomodular law a∨b = a∨(a ⊥ ∧(a∨b)) holds true. The class of OMLs is a variety which contains the variety of Boolean algebras. Moreover, if H is any Hilbert space, then the lattice L(H) of closed subspaces of H, endowed with the usual operation M → M ⊥ , is an OML. If H is finite-dimensional, L(H) is the orthocomplemented modular lattice of all subspaces of H. A block of an OML L is a maximal Boolean subalgebra of L. When L is finite, this algebra can be represented by its Greechie diagram ([12]), a hypergraph, whose vertices correspond to the atoms and whose edges represent the blocks of L. Here we will use such diagrams only in the simplest case described in [11].