Finite-rank operator
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In functional analysis, a branch of mathematics, a finite-rank operator is a bounded linear operator between Banach spaces whose range is finite-dimensional.[1]
Finite-rank operators on a Hilbert space
[edit ]A canonical form
[edit ]Finite-rank operators are matrices (of finite size) transplanted to the infinite dimensional setting. As such, these operators may be described via linear algebra techniques.
From linear algebra, we know that a rectangular matrix, with complex entries, {\displaystyle M\in \mathbb {C} ^{n\times m}} has rank {\displaystyle 1} if and only if {\displaystyle M} is of the form
- {\displaystyle M=\alpha \cdot uv^{*},\quad {\mbox{where}}\quad \|u\|=\|v\|=1\quad {\mbox{and}}\quad \alpha \geq 0.}
Exactly the same argument shows that an operator {\displaystyle T} on a Hilbert space {\displaystyle H} is of rank {\displaystyle 1} if and only if
- {\displaystyle Th=\alpha \langle h,v\rangle u\quad {\mbox{for all}}\quad h\in H,}
where the conditions on {\displaystyle \alpha ,u,v} are the same as in the finite dimensional case.
Therefore, by induction, an operator {\displaystyle T} of finite rank {\displaystyle n} takes the form
- {\displaystyle Th=\sum _{i=1}^{n}\alpha _{i}\langle h,v_{i}\rangle u_{i}\quad {\mbox{for all}}\quad h\in H,}
where {\displaystyle \{u_{i}\}} and {\displaystyle \{v_{i}\}} are orthonormal bases. Notice this is essentially a restatement of singular value decomposition. This can be said to be a canonical form of finite-rank operators.
Generalizing slightly, if {\displaystyle n} is now countably infinite and the sequence of positive numbers {\displaystyle \{\alpha _{i}\}} accumulate only at {\displaystyle 0}, {\displaystyle T} is then a compact operator, and one has the canonical form for compact operators.
Compact operators are trace class only if the series {\textstyle \sum _{i}\alpha _{i}} is convergent; a property that automatically holds for all finite-rank operators.[2]
Algebraic property
[edit ]The family of finite-rank operators {\displaystyle F(H)} on a Hilbert space {\displaystyle H} form a two-sided *-ideal in {\displaystyle L(H)}, the algebra of bounded operators on {\displaystyle H}. In fact it is the minimal element among such ideals, that is, any two-sided *-ideal {\displaystyle I} in {\displaystyle L(H)} must contain the finite-rank operators. This is not hard to prove. Take a non-zero operator {\displaystyle T\in I}, then {\displaystyle Tf=g} for some {\displaystyle f,g\neq 0}. It suffices to have that for any {\displaystyle h,k\in H}, the rank-1 operator {\displaystyle S_{h,k}} that maps {\displaystyle h} to {\displaystyle k} lies in {\displaystyle I}. Define {\displaystyle S_{h,f}} to be the rank-1 operator that maps {\displaystyle h} to {\displaystyle f}, and {\displaystyle S_{g,k}} analogously. Then
- {\displaystyle S_{h,k}=S_{g,k}TS_{h,f},,円}
which means {\displaystyle S_{h,k}} is in {\displaystyle I} and this verifies the claim.
Some examples of two-sided *-ideals in {\displaystyle L(H)} are the trace-class, Hilbert–Schmidt operators, and compact operators. {\displaystyle F(H)} is dense in all three of these ideals, in their respective norms.
Since any two-sided ideal in {\displaystyle L(H)} must contain {\displaystyle F(H)}, the algebra {\displaystyle L(H)} is simple if and only if it is finite dimensional.
Finite-rank operators on a Banach space
[edit ]A finite-rank operator {\displaystyle T:U\to V} between Banach spaces is a bounded operator such that its range is finite dimensional. Just as in the Hilbert space case, it can be written in the form
- {\displaystyle Th=\sum _{i=1}^{n}\langle u_{i},h\rangle v_{i}\quad {\mbox{for all}}\quad h\in U,}
where now {\displaystyle v_{i}\in V}, and {\displaystyle u_{i}\in U'} are bounded linear functionals on the space {\displaystyle U}.
A bounded linear functional is a particular case of a finite-rank operator, namely of rank one.
References
[edit ]- ^ "Finite Rank Operator - an overview". 2004.
- ^ Conway, John B. (1990). A course in functional analysis. New York: Springer-Verlag. pp. 267–268. ISBN 978-0-387-97245-9. OCLC 21195908.