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.
Definition
If
X
{\displaystyle X}
is a vector lattice then by the vector lattice operations we mean the following maps:
- the three maps
X
{\displaystyle X}
to itself defined by x ↦ | x | {\displaystyle x\mapsto |x|}
, x ↦ x + {\displaystyle x\mapsto x^{+}}
, x ↦ x − {\displaystyle x\mapsto x^{-}}
, and
- the two maps from
X
×
X
{\displaystyle X\times X}
into X {\displaystyle X}
defined by ( x , y ) ↦ sup { x , y } {\displaystyle (x,y)\mapsto \sup _{}\{x,y\}}
and ( x , y ) ↦ inf { x , y } {\displaystyle (x,y)\mapsto \inf _{}\{x,y\}}
.
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]
Properties
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]
Examples
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 }
.
See also
- Banach lattice – Banach space with a compatible structure of a lattice
- Complemented lattice – Bound lattice in which every element has a complement
- Fréchet lattice – Topological vector lattice
- Locally convex vector lattice
- Normed lattice
- Ordered vector space – Vector space with a partial order
- Pseudocomplement
- Riesz space – Partially ordered vector space, ordered as a lattice
References
- Schaefer & Wolff 1999, pp. 234–242.
- Schaefer & Wolff 1999, pp. 215–222.
Bibliography
- Narici, Lawrence; Beckenstein, Edward (2011). Topological Vector Spaces. Pure and applied mathematics (Second ed.). Boca Raton, FL: CRC Press. ISBN 978-1584888666. OCLC 144216834.
- Schaefer, Helmut H.; Wolff, Manfred P. (1999). Topological Vector Spaces. GTM. Vol. 8 (Second ed.). New York, NY: Springer New York Imprint Springer. ISBN 978-1-4612-7155-0. OCLC 840278135.