Using Paley-Wiener theorem and Fourier inversion formula to get this result I want to solve the problem #8 of Stein's book Complex analysis in Chapter 4, for the first part I've got the following:
We know that the coefficients of a series are: 
$$a_n=\frac{f^{(n)}(z_0)}{n!}$$
Since the series is centered at $z_0=0$ and using the inverse Fourier transform we get :
$$f^{(n)}=(2 \pi i )^{n} \int_{-\infty}^{\infty}\hat{f}(\zeta)\zeta^{n}e^{2\pi ix\zeta}d\zeta=(2 \pi i )^{n} \int_{-M}^{M}\hat{f}(\zeta)\zeta^{n}e^{2\pi ix\zeta}d\zeta$$
and evaluating at zero and dividing by the factorial we have:
$$a_n=\frac{(2 \pi i )^{n}}{n!} \int_{-M}^{M}\hat{f}(\zeta)\zeta^{n}d\zeta$$
but then I don't know how to bound this to get that 
$$\limsup_{n-> \infty}(n!|a_n|)^{1/n} \le 2 \pi M$$
I was trying to do the following:
$$|a_n|\le \frac{(2 \pi )^n}{n!}\int_{-M}^{M}|\hat{f}(\zeta)||\zeta^{n}|d\zeta$$
the thing is that I don't know how to ensure that the integral is less than $M^n$
Another way I thought of was to use Cauchy's inequalities then I will get the following
$$|a_n| \le \frac{n!}{R^n}||f||_{C}$$
for an appropiate election of the radius of the circle, so I want to pick the circle with center in zero and of radius $M$ but then How can I bound the integral? and I don't think this could take me to the result.
For the second part I don't understand if I can use that $\hat{f}$ is compact supported, if I can then I use Paley- Weiner theorem but I don't know how modify it to get the result since that $\epsilon$ is annoying me. If I can't use it then I can hardly think in a way to prove this.
Can someone help me with this issue please? Thanks in advance.  
 A: You were already on the right track, but stopped a little too soon. You showed
$$
           a_n = \frac{(2\pi i)^{n}}{n!}\int_{-M}^{M}\hat{f}(\zeta)\zeta^n d\zeta
$$
Therefore,
\begin{align}
           (n! |a_n|)^{1/n}&=2\pi\left|\int_{-M}^{M}\hat{f}(\zeta)\zeta^n d\zeta\right|^{1/n} \\
  &\le 2\pi\left(\int_{-M}^{M}|\hat{f}(\zeta)|d\zeta M^{n}\right)^{1/n} \\
  &= 2\pi M\left(\int_{-M}^{M}|\hat{f}(\zeta)|d\zeta\right)^{1/n}
\end{align}
The limit of the right side exists as $n\rightarrow\infty$ and, assuming $\int_{-M}^{M}|\hat{f}(\zeta)|d\zeta \ne 0$, that limit is $2\pi M$. Therefore,
\begin{align}
        \limsup_{n} (n!|a_n|)^{1/n} & \le \limsup_{n} 2\pi M\left(\int_{-M}^{M}|\hat{f}(\zeta)|d\zeta\right)^{1/n} \\ & = \lim_{n}2\pi M\left(\int_{-M}^{M}|\hat{f}(\zeta)|d\zeta\right)^{1/n} = 2\pi M.
\end{align}
The only assumption needed for $\hat{f}$ is that it is absolutely integrable on $[-M,M]$.
For the converse, assume that $f(z)=\sum_{n=0}^{\infty}a_n z^n$, and assume that
$$
    \limsup_{n}(n!|a_n|)^{1/n} \le 2\pi M.
$$
Let $\epsilon > 0$ be given. Then there exists $N$ such that
$$
              \sup_{n \ge N}(n!|a_n|)^{1/n} \le (2\pi M+\epsilon) \\
               n!|a_n| \le (2\pi M+\epsilon)^{n} \;\;\; n \ge N \\
                 \sum_{n=0}^{\infty}|a_n||z|^{n} \le 
        \sum_{n=0}^{N-1}\left(|a_n|-\frac{(2\pi M+\epsilon)^{n}}{n!}\right)|z|^{n}+\sum_{n=N}^{\infty}\frac{1}{n!}(2\pi M+\epsilon)^{n}|z|^{n}
$$
A little juggling of constants to bound the first few terms by the full exponential series gives
$$
        |f(z)| \le C\sum_{n=0}^{\infty}\frac{1}{n!}(2\pi M+\epsilon)^{n}|z|^{n}
   = e^{(2\pi M+\epsilon)|z|}.
$$
A: If $f\in L^1(\mathbb{R})$ then $\hat{f}$ is continuous, and since it is supported in $[-M,M]$, it must be bounded, by some $C>0$. Therefore
$$ n!a_n\leq (2\pi)^n\int_{-M}^M|\hat{f}(t)||t|^n\;dt \leq C(2\pi)^n\int_{-M}^M|t|^n\;dt =\frac{2CM^{n+1}}{n+1}(2\pi )^n$$
Now taking $n$th roots of both sides yields
$$ (n!a_n)^{\frac{1}{n}}\leq \frac{(2CM)^{\frac{1}{n}}}{(n+1)^{\frac{1}{n}}}2\pi M$$
and since $\lim_{n\to\infty}K^{\frac{1}{n}}=1=\lim_{n\to\infty}(n+1)^{\frac{1}{n}}$ for any constant $K$, it follows that
$$ \limsup_{n\to\infty}(n!a_n)^{\frac{1}{n}}\leq2\pi M $$
