Find the Fourier transform of
\left.f(t)\right.=\left\{\begin{array}{l l}{{e^{-3t}}}&{{{t}\mathrm{} \geqslant 0}}\\ {{e^{3t}}}&{{{t}\lt 0}}\end{array}\right.
Deduce the function whose Fourier transform is G(\omega)={\frac{6}{10+2\omega+\omega^{2}}}.
F(\omega)=\int_{-\infty}^{\infty}f(t)\,\mathrm{e}^{-\mathrm{j}\omega t}\,\mathrm{d}t
=\int_{-\infty}^{0}\mathrm{e}^{3t}\,\mathrm{e}^{-\mathrm{j}\omega t}\,\mathrm{d}t+\int_{0}^{\infty}\mathrm{e}^{-3t}\,\mathrm{e}^{-\mathrm{j}\omega t}\,\mathrm{d}t
=\int_{-\infty}^{0}\mathbf{e}^{(3-\mathrm{j}\omega)t}\;\mathrm{d}t\;+\;\int_{0}^{\infty}\mathrm{e}^{-(3+\mathrm{j}\omega)t}\;\mathrm{d}t
=\left[\frac{e^{(3 – j \omega)t} }{3 – j \omega}\right]_{-\infty}^{0} + \left[\frac{e^{-(3 + j \omega)t}}{-(3+j\omega)}\right] _0 ^{\infty}
={\frac{1}{3-\mathrm{j}\omega}}+{\frac{1}{3+\mathrm{j}\omega}}
={\frac{6}{9+\omega^{2}}}
Now
G(\omega)=\frac{6}{10+2\omega+\omega^{2}}=\frac{6}{(\omega+1)^{2}+9}=F(\omega+1)
Then, using the first shift theorem F(ω + 1) will be {\mathcal{F}}\{\mathrm{e}^{-\mathrm{j}t}f(t)\}; that is, the required function is
g(t)=\left\{\begin{array}{l l}{{\mathrm{e}^{(-3-{j})t}}}&{{t\geqslant0}}\\ {{\mathrm{e}^{(3-j)t}}}&{{t\lt 0}}\end{array}\right.