I was wondering about the relationship between the Hankel transform and the Fourier transform for radial functions. Let $f : \mathbb{R}^d \to \mathbb{R}$ be a (sufficiently regular) radial function. The $d$-dimensional Fourier transform is
\begin{align*} \widehat{f}(\xi) &= \int_{\mathbb{R}^d}f(x) e^{-2\pi i \xi \cdot x}\text{d} x\\ &= \int_0^\infty f(r) r^{d-1}\int_{S^{d-1}} e^{-2\pi i r \xi \cdot s}\text{d} s \text{d} r \end{align*} where $f(r)$ denotes the value on the radius-$r$ sphere. This is the integral of $f$ times the function $$ \psi_r(\xi) := r^{d-1}\int_{S^{d-1}} e^{-2\pi i r \xi \cdot s}\text{d} s$$ which is also radial so it's equivalent to a function $\psi_r : \mathbb{R}_{\geq 0} \to \mathbb{R}$.
My question is, do the functions $\psi_r$ have a name? Are they somehow less natural than the Bessel functions?
If I did the calculation correctly, the formula in terms of Bessel functions of the first kind $J_\nu(x)$ is $$ \psi_r(x) = \frac{r^{\frac{d}{2}}\Gamma(\frac d 2)J_{\frac{d-2}{2}}(2\pi rx)}{(\pi x)^{\frac{d-2}{2}}}$$