  For a class of frustrated spin lattices including the kagome lattice we
construct exact eigenstates consisting of several independent, localized
one-magnon states and argue that they are ground states for high magnetic
fields. If the maximal number of local magnons scales with the number of spins
in the system, which is the case for the kagome lattice, the effect persists in
the thermodynamic limit and gives rise to a macroscopic jump in the
zero-temperature magnetization curve just below the saturation field. The
effect decreases with increasing spin quantum number and vanishes in the
classical limit. Thus it is a true macroscopic quantum effect.
