We extend the usual small-polaron theory of diffusion to take into acc
ount states with finite energy width. The possibility of incoherent ho
pping down to T = 0 follows as a direct consequence. Assuming that pos
itive muons in copper are in tunneling states involving just two sites
and resonating with the crystal modes we calculate the temperature de
pendent diffusion coefficient. The results explain quantitatively the
experimental data, including: the anomalous regime occurring at temper
atures below T = 80 K and the flat region close to T = 0. The calculat
ion considers the real vibrational modes of copper, which leads to a r
emarkable agreement between theory and experiment.