explicit solution of fractional laplacian in R^N What is the explicit solution of $(-\Delta)^s u = \chi_{B}$ in $\mathbb{R}^N$ with $0< s<1$ and $\chi$ is the characteristic function and
$B$ is the unit ball around the origin? The answer should follow from the potential theory (answer follows by convolution theory) but I am not getting it in a simple form like the laplacian. Note that by known facts $u$ is continuous and radially symmetric.
 A: The operator $(-\Delta)^s$ in $\mathbb R^N$
is the Fourier multiplier $c_{s,N}\vert \xi\vert^{2s}$, so the Fourier transform of the fundamental solution $E_{s,N}$ should be homogeneous with degree $-2s$, so $E$ should be homogeneous with degree $2s-N$: it is indeed the case for $s=1$ where the fundamental solution of the Laplace equation is, up to a multiplicative constant, $\vert x\vert^{2-N}$ in dimension $\not=2$.
Also that fundamental solution must be radial in the sense that for each vector field $X$ tangential to an Euclidean sphere with center $0$, $XE=0$. A good guess is thus
$$
E_{s,N}(x)=\sigma_{s,N}\vert x\vert^{2s-N}
$$
and a solution of your equation
$$
u(x)=\sigma_{s,N}\int_B\vert x-y\vert^{2s-N} dy.
$$
A: The answer is
$$
u(x) = (-\Delta)^{-\alpha/2} \chi_B(x) = 2^{-\alpha} G_{2,2}^{1,1}\biggl(\begin{matrix}1-(N-\alpha)/2 & 1+\alpha/2 \\ 0 & 1 - N/2\end{matrix} \, \bigg\vert \, |x|^2\biggr) ,
$$
where $G$ is the Meijer G-function; see Corollary 3(i) in this paper. This reduces to the hypergeometric function $_2F_1$; if I copied the expressions correctly from Mathematica, one has:
$$
u(x) = \frac{\Gamma((N-\alpha)/2)}{2^\alpha \Gamma(1+\alpha/2) \Gamma(N/2)} {_2F_1}(-\alpha/2, (N-\alpha)/2; N/2; |x|^2)
$$
for $x \in B$ and
$$
u(x) = \frac{\Gamma((N-\alpha)/2)}{2^\alpha \Gamma(\alpha/2) \Gamma(N/2-\alpha)} |x|^{\alpha-N} {_2F_1}(1-\alpha/2, (N-\alpha)/2; 1+N/2; 1/|x|^2)
$$
for $x \in \mathbb{R}^N \setminus B$. The calculation dates back to Blumenthal–Getoor–Ray (or a subset), I believe.
