If $\mu$ equals Haar measure on the 3-dimensional unit sphere $S^2$, then $\hat{\mu}(\varepsilon) = \dfrac{2\sin(2\pi |\varepsilon|)}{|\varepsilon|}$.
I am not quite sure how to start this problem. First of all, I can't figure out the formula for the $\mu$ itself, let alone computing its Fourier transform. The only I can make sense of $\hat{\mu}$ is when I view $\mu$ as a distribution but even in that case I don't know where to begin with.
Any help is appreciated.
Answer: Here is my attempted solution after looking at given suggestions below. $$\hat{\mu}(\varepsilon) = \int_{S^2} e^{-i\varepsilon\cdot x}dx =4\pi \int_{S^2} e^{-2\pi i\varepsilon\cdot\gamma} d\sigma(\gamma)\, (1)$$, where $d\sigma(\gamma)$ is the surface element of $S^2$. Because $\mu$ is rotationally invariant, so is its Fourier transform. In other words, the above integral is radial in $\varepsilon$. Hence, it suffices to assume that if $|\varepsilon| = \rho$, then $\varepsilon = (0,0,\rho)$. Finally, using routine spherical coordinate transform, we see that our integral in $(1)$ equals to $${4\pi}\int_{0}^{2\pi}\int_{0}^{\pi} e^{-2\pi i\rho\cos\theta}\sin\theta d\theta d\phi = 4\pi\cdot\dfrac{1}{2}\int_{0}^{\pi}e^{-2\pi i\rho\cos\theta}\sin\theta d\theta = $$ $$2\pi\cdot\dfrac{1}{4\pi i\rho}[e^{2\pi i\rho u}]_{u=-1}^{u=1} = \dfrac{2 \sin(2\pi\rho)}{\rho}$$, as desired.
In this case the Haar measure is simply the Lebesgue measure. So you have $$ \hat \mu(\varepsilon)=\int_{S^2} e^{-i\varepsilon x}dx. $$