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Fig. 2.

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Rates of specific kinetic energy diffusion, ⟨ΔE⟩, as a function of the azimuthal velocity, vϕ. The rates are evaluated from Eqs. (A.7) and (A.3) for two values of the stellar velocity dispersion, σ : 20km s1 (in black or grey); and 10 km s1 (in blue or skyblue). A) Setting M = 1 × 107 M, with M/m ≃ 103, the figure graphs each quadratic component and the first-order parallel one (v ⟨Δv⟩, dark solid lines; we note that it has the same sign as RΩ − vϕ). B) The same but for a BH with M = 1 × 108 M (M/mstar ≃ 104). The much higher inertia of the BH leads to a ten-fold increase in the parallel term but only subtle differences in the diffusion (quadratic) ones. The light and dotted-blue curves peak off scale in either case. The (central) angular velocity Ω = 0.05/Myr is such that RΩ ≈ 70km s1 at R = 1.5kpc, a good match to the circular velocity at that radius.

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