Two-dimensional modified Helmholtz fundamental solution (${\Gamma }_m(r)=K_0(mr)/(2\pi )$)

For $m>0$, the decaying fundamental solution of $-\Delta +m^2$ in two dimensions is $K_0(mr)/(2\pi )$, with $K_0$ the Modified Bessel function of the second kind. Green second identity reconstructs an interior solution from its Dirichlet boundary condition $f$ and outward normal derivative $h$ as $q(r)={\int }_{\partial \Omega }({\Gamma }_{m}h-f{\partial }_n{\Gamma }_m)ds$.