Fig. 2.

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Ratio of the contribution to the total cross section from the large-angle regime (dashed lines) and of the modified transfer cross section from the small-angle regime versus the critical angle θc used to separate small- and large-angle regions within the hSIDM scheme for the ‘Møller’ cross section Eq. (1) and r = 102, 103, 104, respectively. Solid lines characterise the expected physical relevance of small-angle scattering (in relative units). For moderate values of θc ≲ 0.5, dashed lines conservatively estimate the expected ratio of the numerical effort of hSIDM compared to a naive implementation of angle-dependent scattering.
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