By expressing the annihilation operator $A$ of the harmonic oscillator in the momentum representation, obtain $\langle p \mid 0\rangle$. Check that your expression agrees with that obtained from the Fourier transform of
$$
\langle x \mid 0\rangle=\frac{1}{\left(2 \pi \ell^{2}\right)^{1 / 4}} \mathrm{e}^{-x^{2} / 4 \ell^{2}}, \quad \text { where } \quad \ell \equiv \sqrt{\frac{\hbar}{2 m \omega}}
$$