This is indeed meant to be a homework question but I just figured out the answer I prepared was false all this time. Kind of panicking, could anyone give me a lift?
$T:\ell^2 \rightarrow \ell^1: Tx = \big( (2^{-k})x_k \big)_{n=1}^{\infty} $
Thanks!
Edit: Here are my thoughts:
Observe that for all $ x \in \ell^2 $ in the unit ball we can attend the bounds $ ||Tx||_{2} = \frac{1}{2}, \frac{1}{4}, \frac{1}{8},... $ Another such bound can be achieved by the series $ (\frac{1}{2^{k/2}})_{j \in \mathbb{N}} $ which goes to $1$. However looking for an upper bound we have
$$ || Tx ||_{1} = \sum_{k=1}^{\infty} | \frac{x_k}{2^k} | $$ which I think naturally should be applied Holder's inequality. I have tried various but non of them would coincide with the lower bounds I gave above.The best I could do was $ 1/\sqrt{3} $ for which I cannot get a lower bound for.
About Hölder and your upper bound, OK: $$ \|Tx\|_1 = \sum_{k=1}^\infty\left|\frac{x_k}{2^k}\right|\le \left(\sum_{k=1}^\infty 2^{-2k}\right)^{1/2} \left(\sum_{k=1}^\infty x_k^2\right)^{1/2} = \frac1{\sqrt 3}\|x\|_2. $$ About finding $x$ with $\|Tx\|_1\approx\frac1{\sqrt 3}\|x\|_2$ (equality can be impossible), see the conditions for equality in the Hölder inequality.