Direct numerical simulations reveal two inertial regions in 3D hall magnetohydrodynamics turbulence, indicating varied statistical properties based on magnetic prandtl number.
We carry out extensive pseudospectral direct numerical simulations (DNSs) of decaying three-dimensional (3D) Hall magnetohydrodynamics (3D HMHD) plasma turbulence at three magnetic Prandtl numbers Prm=0.1, 1.0, and 10.0. Our DNSs have been designed to uncover the dependence of the statistical properties of 3D HMHD turbulence on Prm. We find two different inertial regions: in the first inertial region k<ki∼1/di, both the kinetic-energy and magnetic-energy spectra, Eu(k) and Eb(k), respectively, display power-law regions with an exponent that is consistent with Kolmogorov-type −5/3 scaling, at all values of Prm. In the second inertial region k>ki, the scaling of Eb(k) depends upon Prm. At Prm=0.1, the spectral-scaling exponent is −17/3, but for Prm=1 and 10 this exponent is −11/3. We then show theoretically that Eb(k)∼k−2Eu(k) for Prm≪1 and Eb(k)∼k2Eu(k) for Prm≫1; our DNS results are consistent with our theoretical predictions. We examine, furthermore, left- and right-polarized fluctuations of the fields that lead, respectively, to the dominance of ion-cyclotron or whistler waves. We also show that 3D HMHD turbulence shows signatures of intermittency that we uncover by analyzing the scale dependence of probability distribution functions of velocity- and magnetic-field increments, their structure functions, and their flatness as functions of di and Prm.
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Patel et al. (2025) studied this question.
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