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Magnetorotational instability in Keplerian disks: a nonlocal approacha Lomonosov Moscow State University, Shternberg State Astronomical Institute, Universitetskii prosp. 13, Moscow, 119889, Russian Federation b Kazan Federal University, ul. Kremlyovskaya 18, Kazan, 420008, Russian Federation c Tel-Aviv University, Raymond and Beverly Sackler School of Physics and Astronomy, Tel-Aviv, Israel d Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, Bonn, 53121, Germany We revisit the modal analysis of small perturbations in Keplerian ideal gas flows with a constant vertical magnetic field leading to magnetorotational instability (MRI) using the nonlocal approach. In the general case, MRI modes are described by a Schrödinger-like differential equation with some effective potential, including 'repulsive' (1/r2) and 'attractive' (−1/rr3) terms, and are quantized. In shallow potentials, there are no stationary 'energy levels.' In thin Keplerian accretion discs, the perturbation wavelengths λ =2π /kz are smaller than the disc semi-thickness h only in 'deep' potential wells. We find that there is a critical magnetic field for the MRI to develop. The instability arises for magnetic fields below this critical value. In thin accretion discs, at low background Alfvén velocity cA≪ (cA)cr, the MRI instability increment ω is suppressed compared to the value obtained in the local perturbation analysis, ω ≈ −√3icAkz. We also investigate for the first time the case of a radially variable background magnetic field.
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