Consider the following wave functions, each describing a particle in one dimension and defined over all space (i.e., \(-\infty < x < \infty\)), not confined to an infinite square well.
\(\psi_a(x) = A e^{-x^2/3}\)
\(\psi_b(x) = B \frac{1}{x^2+2} \)
For each wave function: