Given that {\mathcal{F}}\{\delta(t-a)\}=\mathrm{e}^{-\mathrm{j}\omega t} find {\mathcal{F}}\{\mathrm{e}^{-\mathrm{j}ta}\}.
We have f(t) = δ(t − a), F(\omega)=\mathrm{e}^{-\mathrm{j}\omega t}. Applying the t–ω duality principle we find
f(-\omega)=\delta(-\omega-a)={\frac{1}{2\pi}}{\mathcal{F}}\{\mathrm{e}^{-\mathrm{j}ta}\}
Therefore
\begin{array}{c}{{{\mathcal{F}}\{\mathrm{e}^{-\mathrm{j}ta}\}=2\pi\delta(-\omega-a)}}\\ {{\phantom{\qquad}=2\pi\delta(-(\omega+a))}}\\ {{\quad}=2\pi\delta(\omega+a)}\end{array}
since δ(ω) is an even function.