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As the angular variation in δρ becomes more rapid, it acts as a high-pass filter in controlling the strength of each mode with L to δ λ0,b (as indicated by the lower bounding curve of Fig. 4). In the case of the hemispherical δρ, all odd angular momenta bigger than L=1 contributes, and one would expect that the impact of this filtering would amount to suppression of some modes with L≤1 and n∼1. For a distribution with rapid angular variations, the number of such suppressed modes may increase, thereby impacting the convergence of the projection.
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As the angular variation in δρ becomes more rapid, it acts as a high-pass filter in controlling the strength of each mode with L to δ λ0,b (as indicated by the lower bounding curve of Fig. 4). In the case of the hemispherical δρ, all odd angular momenta bigger than L=1 contributes, and one would expect that the impact of this filtering would amount to suppression of some modes with L≤1 and n∼1. For a distribution with rapid angular variations, the number of such suppressed modes may increase, thereby impacting the convergence of the projection.
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