In mathematics, specifically in functional analysis and order theory, a topological vector lattice is a Hausdorff topological vector space (TVS) X {\displaystyle X} that has a partial order ≤ {\displaystyle \,\leq \,} making it into vector lattice that possesses a neighborhood base at the origin consisting of solid sets.[1] Ordered vector lattices have important applications in spectral theory.
If X {\displaystyle X} is a vector lattice then by the vector lattice operations we mean the following maps:
If X {\displaystyle X} is a TVS over the reals and a vector lattice, then X {\displaystyle X} is locally solid if and only if (1) its positive cone is a normal cone, and (2) the vector lattice operations are continuous.[1]
If X {\displaystyle X} is a vector lattice and an ordered topological vector space that is a Fréchet space in which the positive cone is a normal cone, then the lattice operations are continuous.[1]
If X {\displaystyle X} is a topological vector space (TVS) and an ordered vector space then X {\displaystyle X} is called locally solid if X {\displaystyle X} possesses a neighborhood base at the origin consisting of solid sets.[1] A topological vector lattice is a Hausdorff TVS X {\displaystyle X} that has a partial order ≤ {\displaystyle \,\leq \,} making it into vector lattice that is locally solid.[1]
Every topological vector lattice has a closed positive cone and is thus an ordered topological vector space.[1] Let B {\displaystyle {\mathcal {B}}} denote the set of all bounded subsets of a topological vector lattice with positive cone C {\displaystyle C} and for any subset S {\displaystyle S} , let [ S ] C := ( S + C ) ∩ ( S − C ) {\displaystyle [S]_{C}:=(S+C)\cap (S-C)} be the C {\displaystyle C} -saturated hull of S {\displaystyle S} . Then the topological vector lattice's positive cone C {\displaystyle C} is a strict B {\displaystyle {\mathcal {B}}} -cone,[1] where C {\displaystyle C} is a strict B {\displaystyle {\mathcal {B}}} -cone means that { [ B ] C : B ∈ B } {\displaystyle \left\{[B]_{C}:B\in {\mathcal {B}}\right\}} is a fundamental subfamily of B {\displaystyle {\mathcal {B}}} that is, every B ∈ B {\displaystyle B\in {\mathcal {B}}} is contained as a subset of some element of { [ B ] C : B ∈ B } {\displaystyle \left\{[B]_{C}:B\in {\mathcal {B}}\right\}} ).[2]
If a topological vector lattice X {\displaystyle X} is order complete then every band is closed in X {\displaystyle X} .[1]
The Lp spaces ( 1 ≤ p ≤ ∞ {\displaystyle 1\leq p\leq \infty } ) are Banach lattices under their canonical orderings. These spaces are order complete for p < ∞ {\displaystyle p<\infty } .