In many ways, the progression of our understanding of the seismic radiation pattern of earthquakes has mirrored the evolution of earthquake science itself. By the early 1900s (Reid, 1911), it was well understood that earthquakes represented shear slip on faults at depth within the Earth's crust. However, connecting this heuristic understanding with more sophisticated theoretical models of the earthquake source proved surprisingly difficult. In the 1920s, Nakano (1923) suggested that the recorded ground motions from earthquakes may be explained by a double-couple representation of the earthquake source. This hypothesis remained controversial for nearly 40 yr, until a series of theoretical and observational studies (Balakina et al., 1961;Burridge & Knopoff, 1964;Honda, 1962;Vvedenskaya, 1956), combined with routine estimation of earthquake mechanisms made possible through the advent of the World-Wide Network of Seismograph Stations (Oliver & Murphy, 1971) definitively demonstrated the double-couple model's validity. To this day, knowledge of the radiation pattern of a double-couple source is fundamental to many problems in seismology and is thus a cornerstone of many introductory classes in earthquake science.While it is widely acknowledged that real earthquake sources may deviate from a theoretical double couple in important ways (Frohlich, 1994;Hayashida et al., 2020;Julian et al., 1998), the double-couple model has proven remarkably successful in explaining the radiation pattern of earthquakes at long periods (frequencies < ∼2 Hz). At higher frequencies, however, the situation becomes more complicated and the model notably less satisfactory (Castro et al., 2006). The effects of scattering become more pronounced at higher