Wave Properties of particles. Schrodinger Equation.
Problem 6.84
Using the Schrödinger equation, demonstrate that at the point where the potential energy U(x) of a particle has a finite discontinuity, the wave function remains smooth, i.e. its first derivative with respect to the coordinate is continuous.
6.84. Let us integrate the Schrödinger equation over a small interval of the coordinate x within which there is a discontinuity in U(x), for example at the point x=0 : ∂x∂ψ(+δ)−∂x∂ψ(−δ)=∫−8+8ℏ22m(E−U)ψdx Since the discontinuity U is finite the integral tends to zero as δ→0. What follows is obvious.