  We study the effect of spin-phonon coupling in small magnetic clusters,
concentrating on a S=1/2 ring of 4 spins coupled antiferromagnetically. If the
phonons are treated as classical variables, there is a critical value of the
spin-phonon coupling above which a static distortion occurs. This is a good
approximation if the zero point energy is small compared to the energy gain due
to the distortion, which is true for large exchange interactions compared to
the phonons energy ($J\gg\hbar\omega$). In the opposite limit, one can
integrate out the phonon degrees of freedom and get an effective spin
hamiltonian. Using exact diagonalizations to include the quantum nature of both
spins and phonons, we obtain the spectrum in the whole range of parameters and
explicit the crossover between the classical and quantum regimes. We then
establish quantitatively the limits of validity of two widely used approaches
(one in the quantum and one in the classical limits) and show that they are
quite poor for small magnetic clusters. We also show that upon reducing
$\hbar\omega/J$ the first excitation of a 4-site cluster becomes a singlet, a
result that could be relevant for Cu$_2$Te$_2$O$_5$Br$_2$.
