Nevertheless, non-interferometric experiments reported in ref. (see also discussion in ref. ), based on radiation emission of charged particles during the collapse, go in a different direction: They claim that the width of the mass distribution should be at least one order of magnitude broader than the nuclear wave function. For instance, for germanium atoms, the material they measured, they claimed that the mass distribution width must be bigger than R0 = 0.54 Å (where, in their model, R0 is the radius of a rigid sphere representing the nucleus). In contrast, using the fitting proposed in Table (with Rat = 2.34 Å as given in ref. ), the Gaussian standard deviation would be RN = 0.07 Å. Comparing the sphere and the Gaussian radius is somewhat arbitrary. Still, if we overlook it, it is clear that RN is smaller than the lower bound width R0.