Fig. 5.

Dynamical friction against the perturber mass M, for V = 1.5cT = 0, with the results from finite-time linear perturbation theory included with dotted lines of the same colors. The departure from perturbation theory for the zero-temperature case at high M is due to nonlinear effects. Increasing the mass of the perturber causes the superfluid to behave increasingly like a normal fluid, similarly to the effect of decreasing .
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