Abstract:
The nonstationary wave function $\Psi_k(x, T)$ with initial condition $\Psi_k(x, 0)=\exp(ikx)$ and stationary wave function $\psi_k(x)$ of the scattering problem are represented by functional integrals. This representation is used in the three-dimensional problem of scattering on an arbitrary (not necessarily central) potential to obtain the quasiclassical scattering amplitude and also the quantum corrections to it.