Fourier transform periodic signal I have to find the Fourier transform is this signal $ \sum_{n= - \infty }^{+ \infty }  e^{- 2 \pi | \frac{t-nT_0}{T_0} |} $
I know that the Fourier transform of $ \sum_{n= - \infty }^{+ \infty } x_0 (t-nT) $ Is $ X_0(kf_0) f_0 \delta (f- kf_0)$ . Now I have to find $ X_0(kf_0)$ and $ X_0 (f) $
I know that the Fourier transform of $ e^{-a|t|} $ Is $ \frac{2a}{a^{2} + w^{2} }$
So the Fourier transform Of $ e^{- 2 \pi | \frac{t-nT_0}{T_0} |} $ , also written as $ e^{-2\pi |\frac{t}{T_0} - n| } $ , should be $ \frac{ 4 T_0 \pi }{4 (\pi )^{2} + w^{2} } $
Now I Find   $ X(k f_0) $ with  $ f= kf_0 $ , and I obtain $ X(k f_0) = \frac {T_0}{\pi + \pi k^{2} f_0^{2} } $
Finally , I obtained that $ X(f) = \frac {1}{\pi} \frac {1}{1 + k^{2} f_0 ^{2} } \delta(f- kf_0 ) $ But the result on my book is $ X(f) = \frac {1}{\pi} \frac {1}{1 + k^{2} } \delta(f- kf_0 ) $
 A: Rephrasing your question:

Prove that
$$x(t)=\sum_{n=-\infty}^{+\infty}e^{-2\pi\left|\frac{t-nT_0}{T_0}\right|}\xrightarrow{\text{FT}}X(f)=\frac{1}{\pi}\left(\frac1{1+k^2}\right)\delta(f-kf_0)$$
, given that $k=f/f_0$, $T_0f_0=1$, where $T_0>0$, $n\in \mathbb{Z}$.

Solution:
Let Fourier transform of $x(t)=e^{\frac{-2\pi}{|T_0|}|t-nT_0|}$ be $X(f)$ and that of $x^\prime(t)=e^{\frac{-2\pi}{|T_0|}|t|}$ be $X^\prime(f)$.
Time-shifting property of Fourier transform
\begin{align*}
y(t\pm t_0)&\xrightarrow{\text{FT}} Y(f)e^{\pm j2\pi ft_0}\\
\text{if}\quad y(t)&\xrightarrow{\text{FT}}Y(f)
\end{align*}
So, $$e^{\frac{-2\pi}{|T_0|}|t-nT_0|}\xrightarrow{\text{FT}} X^\prime(f)e^{-j2\pi fnT_0}\tag{1}$$
You know that
$$e^{-a|t|}\xrightarrow{\text{FT}} \frac{2a}{a^2+(2\pi f)^2}$$
So, $$e^{\frac{-2\pi}{|T_0|}|t|}\xrightarrow{\text{FT}}\frac{\frac{4\pi}{|T_0|}}{\left(\frac{2\pi}{|T_0|}\right)^2+(2\pi f)^2}\equiv \frac1{\pi |T_0|}\left(\frac1{\frac1{(T_0)^2}+f^2}\right)\tag{2}$$
From equation $(1)$ and $(2)$, we get
$$e^{\frac{-2\pi}{|T_0|}|t-nT_0|}\xrightarrow{\text{FT}} \frac1{\pi |T_0|}\left(\frac1{\frac1{(T_0)^2}+f^2}\right)e^{-j2\pi fnT_0}\tag{3}$$
On summating equation $(3)$ over all integers $n$, we get
$$\sum_{n=-\infty}^{+\infty}e^{\frac{-2\pi}{|T_0|}|t-nT_0|}\xrightarrow{\text{FT}} \frac1{\pi |T_0|}\left(\frac1{\frac1{(T_0)^2}+f^2}\right)\sum_{n=-\infty}^{+\infty}e^{-j2\pi fnT_0}=\frac{f_0}{\pi}\left(\frac1{f_0^2+f^2}\right)\sum_{n=-\infty}^{+\infty}e^{+j2\pi fnT_0}\equiv \frac{1}{\pi f_0}\left(\frac1{1+\left(\frac{f}{f_0}\right)^2}\right)\sum_{n=-\infty}^{+\infty}e^{+j2\pi fnT_0}\quad\quad(\because n\in (-\infty,+\infty)\text{ and }T_0f_0=1) \tag{4}$$
We know that the Fourier series of an impulse train is
$$\sum_{n=-\infty}^{+\infty}\delta(t-nT)=\frac1{T}\sum_{n=-\infty}^{+\infty}e^{j2\pi nt/T}\tag{5}$$
Finding an impulse train that could divert the RHS of equation $(4)$ towards the answer by replacing $t\rightarrow f$ and $T\rightarrow f_0$:
$$\sum_{n=-\infty}^{+\infty}\delta(f-nf_0)=\frac1{f_0}\sum_{n=-\infty}^{+\infty}e^{j2\pi nf/f_0}\tag{6}$$
Replacing $k\rightarrow f/f_0$ and substituting equation $(6)$ in equation $(4)$, we get
$$\sum_{n=-\infty}^{+\infty}e^{\frac{-2\pi}{|T_0|}|t-nT_0|}\xrightarrow{\text{FT}} \frac{1}{\pi}\left(\frac1{1+\left(\frac{f}{f_0}\right)^2}\right)\sum_{n=-\infty}^{+\infty}\delta(f-nf_0)=\frac{1}{\pi}\left(\frac1{1+k^2}\right)\delta(f-kf_0)\quad\quad(\because \delta(f-nf_0)=0\ \forall\ n \neq k)$$
(Hence proved :))
