Tuesday, July 26, 2016

measure theory - Finding the norm of the operator Mg:LptoLp where ginLinfty




Suppose (X,A,μ) is a measure space where μ is a finite measure, and p(1,). Say that we take some gL, and we define Mg:LpLp by Mg(f)=fg. Then I'd like to show that ||Mg||=||g||. I'm not absolutely sure this is true, but I think it is. I've shown that ||Mg||||g||, which is pretty simple, but now I'd like to find a function fLp such that ||Mg(f)||p||f||p=||g||. Here's what I've got so far:



Let M=||g||, the essential supremum of |g|. Then let N be the subset of X on which |g(x)|<M2. Now 0<μ(N)<μ(X)< and 0<μ(XN)< too. These things follow from the definition of M and the fact that μ is a finite measure. So define f:XR as
f(x)={0xNM|g(x)|(μ(XN))1pxXN.




Then ||Mg(f)||pp=XNMpμ(XN)dμ=Mp, so||Mg(f)||p=M.



And we can easily show that fLp because M|g(x)| is not going to blow up when |g(x)|M2.



However, we don't have ||f||p=1, so we only have ||Mg(f)||p=M, not ||Mg(f)||p||f||p=M as we require.



So the question is, can this example be tweaked easily to get a unit-normed f satisfying ||Mg(f)||p=M, or is the whole thing off track?


Answer




With some small modifications, your proof can be converted into a working proof.



Instead of using |g(x)|<M2, we use
|g(x)|<Ma, where a>1 is arbitrary.
Then, the rest of the proof can be repeated as you did.



We have to calculate :
\begin{aligned} \|f\|_p^p & = \int_{X\setminus N} \frac{M^p}{|g(x)|^p \mu(X\setminus N)} \mathrm d\mu \\ & \leq \int_{X\setminus N} \frac{M^p}{(M/a)^p \mu(X\setminus N)} \mathrm d\mu \\ & \leq \mu(X\setminus N) \frac{M^p}{(M/a)^p \mu(X\setminus N)} \\ & = a^p \end{aligned}



So \|f\|_p\leq a.




Then we have
\frac{\|M_g(f)\|_p}{\|f\|_p} = \frac{M}{\|f\|_p} \geq \frac{M}{a}.



Because a can be arbitrarily close to 1, this completes the proof.



Note that because of the \sup in the definition of the operator norm, you do not need to show that

\frac{\|M_g(f)\|_p}{\|f\|_p} = M,
only that you can find functions f such that
\frac{\|M_g(f)\|_p}{\|f\|_p}
is arbitrarily close to M.


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