Fig. 10.
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(a) Radial and (b) polar components of the neutron velocity for θ = π/3 and θ = π/2 as functions of r for the magnetic field model II using the HHJ EoS. The evaluation is done semi-analytically (corresponding to ζ = 0; continuous line) and numerically, using the FF approach with Dedalus (dashed line) and our finite difference code (dotted line), both using ζ = 10−3.
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