  A classic route for destroying long-lived electronic quasiparticles in a
weakly interacting Fermi liquid is to couple them to other low-energy degrees
of freedom that effectively act as a bath. We consider here the problem of
electrons scattering off the spin fluctuations of a geometrically frustrated
antiferromagnet, whose non-linear Landau-Lifshitz dynamics, which remains
non-trivial at all temperatures, we model in detail. At intermediate
temperatures and in the absence of any magnetic ordering, the fluctuating
local-moments lead to a non-trivial angular anisotropy of the scattering-rate
along the Fermi surface, which disappears with increasing temperature,
elucidating the role of "hot-spots". Over a remarkably broad window of
intermediate and high temperatures, the electronic properties can be described
by employing a local approximation for the dynamical spin-response. This we
contrast with the more familiar setup of electrons scattering off classical
phonons, whose high-temperature limit differs fundamentally on account of their
unbounded Hilbert space. We place our results in the context of layered
magnetic delafossite compounds.
