Impulse Response Question
As Dilip pointed out in the comment above, you can get the impulse response using the inverse Fourier transform. However, a slightly easier method might be to use the Laplace domain instead; it's more amenable to easy inverse transforming via transform tables. First, recall that the frequency response is really just the $s$-plane transfer function evaluated along the imaginary axis. That is:

$$
H(j\omega) = H(s)|_{s=j\omega}
$$

Go through your frequency response expression and substitute $s$ back in for $j\omega$:

$$
\begin{align}
H(j\omega) &amp;= \frac{1}{-\omega^2+3j\omega+2} \\
&amp;= \frac{1}{(j\omega)^2+3j\omega+2} \\
\end{align}
$$

$$
H(s) = \frac{1}{s^2+3s+2}
$$

So now we have the transfer function in the $s$-plane. To get from here to an easily-inverse-transformable expression, we use a partial fraction decomposition on the transfer function (an online calculator is available here:

$$
H(s) = \frac{1}{s+1} + \frac{1}{s+2}
$$

Given this form, we now refer to a table of common Laplace transforms to find:

$$
e^{-\alpha t} u(t) \Leftrightarrow \frac{1}{s+\alpha}
$$

where $u(t)$ is the Heaviside step function. The impulse response of the system is the inverse Laplace transform of its transfer function. Using the linearity of the Laplace transform and the above relation, we can therefore conclude that:

$$
h(t) = u(t) \left(e^{-t} + e^{-2t} \right)
$$