The Dirac delta function \( \delta(t - t_0) \) has the property that for a test function \( \varphi(t) \), the integral involving the delta function evaluates to \( \varphi(t_0) \) if \( t_0 \) lies between the limits of integration, and zero otherwise. This is known as the sifting property of the delta function.
Now, we need to find the Laplace transform of \( \delta(t - a) \), which is defined as:
\[
\mathcal{L}(\delta(t - a)) = \int_0^\infty e^{-st} \delta(t - a) \, dt
\]
Using the sifting property, we get:
\[
\mathcal{L}(\delta(t - a)) = e^{-sa}
\]
Thus, the correct Laplace transform of \( \delta(t - a) \) is \( e^{-sa} \).
Final Answer: (D)