In the Thom's approach to the classification of instabilities in one-dimensional classical systems every equilibrium is assigned a local minimum in one of the Arnold's benchmark potentials V (k) (x) = x k+1 + c 1 x k−1 + . . .. We claim that in quantum theory, due to the tunneling, the genuine catastrophes (in fact, abrupt "relocalizations" caused by a minor change of parameters) can occur when the number N of the sufficiently high barriers in the Arnold's potential becomes larger than one. A systematic classification of the catastrophes is then offered using the variable mass term 2 /(2µ), odd exponents k = 2N + 1 and symmetry assumption V (k) (x) = V (k) (−x). The goal is achieved via a symbolic-manipulation-based explicit reparametrization of the couplings c j . At the not too large N, a surprisingly user-friendly recipe for a systematic determination of parameters of the catastrophes is obtained and discussed. 1 znojil@ujf.cas.cz