You already have a correct answer, but I'd like to show you a little trick that allows you to derive the solution without solving any integrals. You've already figured out the analytical expression for $X_1(j\omega)$, which is an important step. Now you could observe that this expression contains a factor $j\omega$. Remember that multiplication by $j\omega$ in the frequency domain corresponds to differentiation in the time domain:
$$\mathcal{F}\left\{\frac{dx(t)}{dt}\right\}\Longleftrightarrow j\omega X(j\omega)\tag{1}$$
This means that you could obtain the function $x_1(t)$ by first deriving the inverse Fourier transform of
$$X(j\omega)=\frac{X_1(j\omega)}{j\omega}=3[u(\omega+3\pi)-u(\omega-3\pi)]\tag{2}$$
which is a simple rectangular function. It's corresponding time domain function is
$$x(t)=\frac{3\sin(3\pi t)}{\pi t}\tag{3}$$
This is a basic Fourier transform relationship, which you should know by heart.
The desired function $x_1(t)$ is now given by the derivative of $(3)$:
$$\begin{align}x_1(t)=\frac{dx(t)}{dt}&=\frac{(3\pi)^2 t\cos(3\pi t))-3\pi\sin(3\pi t))}{(\pi t)^2}\\&=\frac{3}{\pi t^2}[3\pi t\cos(3\pi t)-\sin(3\pi t)]\tag{4}\end{align}$$