A free particle of energy $E$ approaches a square, one-dimensional potential well of depth $V_{0}$ and width $2 a$. Show that the probability of being reflected by the well vanishes when $K a=n \pi / 2$, where $n$ is an integer and $K=\left(2 m\left(E+V_{0}\right) / \hbar^{2}\right)^{1 / 2}$. Explain this phenomenon in physical terms.