Figure 12
Angle of arrival of 40 s Rayleigh waves at PAF as a function of backazimuth at the station, for a representative selection of events in Table 1. The angle is measured positive clockwise with respect to the direction of the epicentre–station great circle and is calculated in the phase velocity model of Trampert & Woodhouse (1997).

Angle of arrival of 40 s Rayleigh waves at PAF as a function of backazimuth at the station, for a representative selection of events in Table 1. The angle is measured positive clockwise with respect to the direction of the epicentre–station great circle and is calculated in the phase velocity model of Trampert & Woodhouse (1997).

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