We study the chaotic dynamics in a classical many-body system of interacting
spins on the kagome lattice. We characterise many-body chaos via the butterfly
effect as captured by an appropriate out-of-time-ordered correlator. Due to the
emergence of a spin liquid phase, the chaotic dynamics extends all the way to
zero temperature. We thus determine the full temperature dependence of two
complementary aspects of the butterfly effect: the Lyapunov exponent, μ,
and the butterfly speed, vb, and study their interrelations with usual
measures of spin dynamics such as the spin-diffusion constant, D and
spin-autocorrelation time, τ. We find that they all exhibit power law
behaviour at low temperature, consistent with scaling of the form D∼vb2/μ and τ−1∼T. The vanishing of μ∼T0.48 is
parametrically slower than that of the corresponding quantum bound, μ∼T, raising interesting questions regarding the semi-classical limit of such
spin systems.Comment: 6+4 pages, 4+8 figures, ancillary files include videos of the
dynamic