S U M M A R YWe extended a high-order finite-difference scheme for the elastic SH-wave equation in axisymmetric media for use on parallel computers with distributed memory architecture. Moreover, we derive an analytical description of the implemented ring source and compare it quantitatively with a double couple source. The restriction to axisymmetry and the use of high performance computers and PC networks allows computation of synthetic seismograms at dominant periods down to 2.5 s for global mantle models. We give a description of our algorithm (SHaxi) and its verification against an analytical solution. As an application, we compute synthetic seismograms for global mantle models with additional stochastic perturbations applied to the background S-wave velocity model. We investigate the influence of the perturbations on the SH wavefield for a suite of models with varying perturbation amplitudes, correlation length scales, and spectral characteristics. The inclusion of stochastic perturbations in the models broadens the pulse width of teleseismic body wave arrivals and delays their peak arrival times. Coda wave energy is also generated which is observed as additional energy after prominent body wave arrivals. The SHaxi method has proven to be a valuable method for computing global synthetic seismograms at high frequencies and for studying the seismic waveform effects from models where rotational symmetry may be assumed.Despite the ongoing increase of computational performance, full 3-D global seismic waveform modelling is still a challenge and far from being a routine tool for understanding the Earth's interior. Yet, for teleseismic distances, a substantial part of the seismic energy travels in the great circle plane between source and receiver and can be approximated assuming invariance in the out of plane direction. This motivates algorithms which take advantage of this invariance with a much higher efficiency compared to full 3-D methods. A straightforward realization is to ignore the out of plane direction and compute the wavefield along the two remaining dimensions. For example, Furumura et al. (1998) developed a pseudospectral scheme in cylindrical coordinates and invariance in the direction parallel to the axis of the cylinder for modelling P-SV wave propagation down to depths of 5000 km. This geometry corresponds to a physical