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Fig. 10

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Oscillation frequency of the torus as a function of the black-hole dimensionless spin a from the numerical simulation (assuming 0 ≤ a ≤ 1, q = 1). Different runs differ from each other by the radial position of the centre of the accretion torus, and therefore the oscillation frequency also varies. The functional dependence agrees with the radial epicyclic mode.

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