0.1.13 Transform the ODE - dr² d²y(r) k²y(r) + Voy(r) -r -y(r) = 0 10.2 Problems in Two and Three Dimensions and the boundary conditions y(0) = y(00) = 0 into an integral equation of the form ∞ 459 y(r) = -Vo ;f). 0 The quantities Vo and k² are constants. The ODE is derived from the Schrödinger wave equation with a mesonic potential: 1 e sinh kr, 0<r<t, k G(r,t) = e sinhkt, t<r<∞. k