Fig. 9.

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Intrinsic CR diffusion coefficient, κcr, for simulations utilising two-moment CR transport with varying initial values of Xcr, 0. Scatter points represent the distribution of CRs as a function of κcr and Xcr at t=6 tcool, with darker colours indicating higher CR-energy-weighted probability density in a logarithmic colour scheme. The corresponding 1D probability density of κcr is displayed with a linear scaling on the right-hand side. In the regime of efficient CR scattering (small κcr), larger Xcr, 0 values increase the overall CR energy density in the CGM allowing for more CR energy to be converted into gyroresonant Alfvén waves and larger CR scattering rates, thereby reducing κcr (see Eq. (13)). In regions of a smooth CR distribution, the driving of Alfvén waves is inefficient in comparison to wave damping processes so that CRs are poorly coupled to the plasma, leading to a very large value of κcr.
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