In mathematics, specifically in order theory and functional analysis, two elements x and y of a vector lattice X are lattice disjoint or simply disjoint if
, in which case we write
, where the absolute value of x is defined to be
.
We say that two sets A and B are lattice disjoint or disjoint if a and b are disjoint for all a in A and all b in B, in which case we write
.
If A is the singleton set
then we will write
in place of
.
For any set A, we define the disjoint complement to be the set
.
Characterizations
Two elements x and y are disjoint if and only if
.
If x and y are disjoint then
and
, where for any element z,
and
.
Properties
Disjoint complements are always bands, but the converse is not true in general.
If A is a subset of X such that
exists, and if B is a subset lattice in X that is disjoint from A, then B is a lattice disjoint from
.
Representation as a disjoint sum of positive elements
For any x in X, let
and
, where note that both of these elements are
and
with
.
Then
and
are disjoint, and
is the unique representation of x as the difference of disjoint elements that are
.
For all x and y in X,
and
.
If y ≥ 0 and x ≤ y then x+ ≤ y.
Moreover,
if and only if
and
.
See also
References
Sources
- Schaefer, Helmut H.; Wolff, Manfred P. (1999). Topological Vector Spaces. GTM. Vol. 3. New York, NY: Springer New York Imprint Springer. ISBN 978-1-4612-7155-0. OCLC 840278135.
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| Basic concepts | |
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| Types of orders/spaces | |
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| Types of elements/subsets | |
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| Topologies/Convergence | |
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| Operators | |
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| Main results | |
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