Abstract

Space and astrophysical plasmas often develop into a turbulent state and exhibit nearly random and stochastic motions. While earlier studies emphasize more on understanding the energy spectrum of turbulence in the one-dimensional context (either in the frequency or the wavenumber domain), recent achievements in plasma turbulence studies provide an increasing amount of evidence that plasma turbulence is essentially a spatially and temporally evolving phenomenon. This review presents various models for the space–time structure and anisotropy of the turbulent fields in space plasmas, or equivalently the energy spectra in the wavenumber–frequency domain for the space–time structures and that in the wavevector domain for the anisotropies. The turbulence energy spectra are evaluated in different one-dimensional spectral domains; one speaks of the frequency spectra in the spacecraft observations and the wavenumber spectra in the numerical simulation studies. The notion of the wavenumber–frequency spectrum offers a more comprehensive picture of the turbulent fields, and good models can explain the one-dimensional spectra in the both domains at the same time. To achieve this goal, the Doppler shift, the Doppler broadening, linear-mode dispersion relations, and sideband waves are reviewed. The energy spectra are then extended to the wavevector domain spanning the directions parallel and perpendicular to the large-scale magnetic field. By doing so, the change in the spectral index at different projections onto the one-dimensional spectral domain can be explained in a simpler way.

Highlights

  • Page 3 of 48 2 as a power-law spectrum for a realization of the inertial range by Kolmogorov (1991)

  • This review presents various models for the space–time structure and anisotropy of the turbulent fields in space plasmas, or equivalently the energy spectra in the wavenumber–frequency domain for the space–time structures and that in the wavevector domain for the anisotropies

  • Laminar flows are representative for low Reynolds numbers, while turbulent flows occur at high Reynolds numbers (Frisch 1995)

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Summary

Page 2 of 48

Space–time structure and wavevector anisotropy in space. Page 3 of 48 2 as a power-law spectrum for a realization of the inertial range by Kolmogorov (1991). One is the scale invariance and the other is isotropy Both of them are the properties of Navier–Stokes equation in the inviscid limit (zero viscosity limit), e.g., Frisch (1995). These two properties are related to the scaling symmetry and the rotation symmetry in the fluid system. Transition from a laminar to a turbulent flow can conveniently be characterized by evaluating the Reynolds number, Re. Here U is the characteristic flow speed in the system, L the characteristic length scale, and ν the viscosity of the medium. Due to the vast length scale L and the small viscosity ν, the plasmas in the solar system and astrophysical systems are characterized by very large Reynolds numbers.

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Magnetohydrodynamic picture
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Kinetic waves
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Alfvén mode family
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Fast mode family
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Slow mode family
Zero-frequency mode
Sideband waves
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Coherent structures
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Lessons from the observations
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Impact of the large-scale magnetic field
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Two-component model
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Critical balance model
Elliptic anisotropy model
Non-elliptic anisotropy model
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Asymmetries
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Findings
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Full Text
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