Abstract
We use the Schwinger-boson mean-field theory to study the spin dynamics of Heisenberg magnets in which quantum (finite S) fluctuations have destroyed the classical Néel long-range order. The low-temperature physics is dominated by the zone-center gap Δ(T) which remains finite as T->0. The effect of this T-dependent low-energy cutoff on the magnetic response functions (susceptibilty, structure factor, relaxation rates) is analyzed. We use this model to discuss the validity of a description of antiferromagnetic fluctuations in YBa2 Cu3 O6+x in terms of local moments.