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Let $m$ be Lebesgue measure on $[0,1]$ and define $||f||_p$ with respect to $m$ as usual. What are all functions $\Phi$ on $[0, \infty)$ such that the relation

$$ \Phi( \lim_{p\to\ 0}||f||_p)= \int_{0}^{1}(\Phi\circ f)dm$$ holds for every bounded, measurable, positive $f$ ?

A hint is provided:

Show first that $$c \Phi(x)+(1-c) \Phi(1)= \Phi(x^c) \ \ (x>0, 0 \le c \le 1) \ \tag 1 $$

I was thinking of using this $$ \lim_{p\to\ 0}||f||_p = \exp\left \{ \int_0^1 \log |f| dm\right \}$$ From here we get that $\log $ satisfies the condition.

Then I tried to show that any $\Phi$ which meets the conditions of $(1)$ must satisfy the relation, $\Phi(xy)= \Phi(x)+ \Phi(y)$ from which I want to conclude that $log$ is the only such function.

Is my line of thinking correct? If not, then how should I proceed?

Hirshy
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Epsilon
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1 Answers1

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First, it's not clear from your post and the comments whether you've seen why $\Phi$ must satisfy (1). Let $f=x\chi_{(0,c)}+\chi_{(c,1)}$. Then $$\int_0^1\Phi(f)=c\Phi(x)+(1-c)\Phi(1),$$while $$||f||_p=\left(cx^p+1-c\right)^{1/p}.$$ So $$\log(||f||_p)=\frac1p\log(1+c(x^p-1))\sim\frac cp\left(e^{p\log(x)}-1\right)\sim c\log(x).$$So (1) holds.

Now if you let $\Psi(s)=\Phi(e^s)-\Phi(1)$ then (1) gives $$c\Psi(t)=\Psi(ct)\quad(0\le c\le 1,\,t\in\Bbb R).$$Setting $t=1$ shows that $$\Psi(c)=c\Psi(1)\quad(0\le c\le 1).$$And $t=2$ shows $\Psi(2c)=2\Psi(c)$. Hence $$\Psi(c)=c\Psi(1)\quad(c\ge0).$$

Unravelling things now shows that $\Phi(t)$ is a linear combination of $1$ and $\log(t)$.


Conversely, any linear combination of $1$ and $\log$ works. This is well known, or at least better known to me than what's above. Proofs exist in various places, for example On the space $L^0$ and $\lim_{p \to 0} \|f\|_p$ . (Ok, all you actually find there is a proof that $\Phi=\log$ works. But it's obvious that $\Phi=1$ works, and that the set of $\Phi$s that work is closed under linear combinations.)

  • Why did you take this specific $f$? Could you explain it? It does not look like a general proof. – Epsilon Oct 14 '15 at 12:02
  • @VaibhavJena We are given that $\Phi(\lim||f||p)=\int\Phi\circ f$ for _every $f$. In particular that holds for the $f$ that I chose. It holds for any $f$. The reason I chose that particular $f$ is that it shows how what we are given implies (1). It is true that I didn't show that in fact if $\Phi$ is a linear combination of $1$ and $\log$ then $\Phi(\lim||f||_p)=\int\Phi\circ f$ holds for every $f$. That's not part of what the problem asked us to prove. (There are various posts around here, including one by me, that do show that any linear combination of $1$ and $\log$ works.) – David C. Ullrich Oct 14 '15 at 13:23
  • But can we say that there does not exist any other function apart from linear, $\log$ and their combinations ? – Epsilon Oct 14 '15 at 13:37
  • @VaibhavJena Yes, we can say there are no other such functions. That's exactly what I proved. Come to think of it I should retract my previous comment, though: Looking back at the question, it said "find all $\Phi$ such that...". I showed that if $\Phi$ works then $\Phi$ is a linear combination of $1$ and $\log$, but yes the question does require that we also show that any linear combination of $1$ and $\log$ works. – David C. Ullrich Oct 14 '15 at 13:42
  • @VaibhavJena I just edited this post to include it. Thanks for pointing out the gap... – David C. Ullrich Oct 14 '15 at 13:48