Abstract

Kink oscillations of coronal loops, i.e., standing kink waves, is one of the most studied dynamic phenomena in the solar corona. The oscillations are excited by impulsive energy releases, such as low coronal eruptions. Typical periods of the oscillations are from a few to several minutes, and are found to increase linearly with the increase in the major radius of the oscillating loops. It clearly demonstrates that kink oscillations are natural modes of the loops, and can be described as standing fast magnetoacoustic waves with the wavelength determined by the length of the loop. Kink oscillations are observed in two different regimes. In the rapidly decaying regime, the apparent displacement amplitude reaches several minor radii of the loop. The damping time which is about several oscillation periods decreases with the increase in the oscillation amplitude, suggesting a nonlinear nature of the damping. In the decayless regime, the amplitudes are smaller than a minor radius, and the driver is still debated. The review summarises major findings obtained during the last decade, and covers both observational and theoretical results. Observational results include creation and analysis of comprehensive catalogues of the oscillation events, and detection of kink oscillations with imaging and spectral instruments in the EUV and microwave bands. Theoretical results include various approaches to modelling in terms of the magnetohydrodynamic wave theory. Properties of kink oscillations are found to depend on parameters of the oscillating loop, such as the magnetic twist, stratification, steady flows, temperature variations and so on, which make kink oscillations a natural probe of these parameters by the method of magnetohydrodynamic seismology.

Highlights

  • One of the key features which makes the plasma of the solar corona different from other natural plasma environments, for example, the Earth’s magnetosphere, is a pronounced fieldaligned filamentation of the macroscopic parameters, such as the density and temperature.Oscillatory Processes in Solar and Stellar Coronae Edited by Valery M

  • The model that has proven to be standard in the kink oscillation modelling is based on linear MHD perturbations of a plasma cylinder surrounded by a plasma with different properties, with both the internal and external plasmas being penetrated by a straight magnetic field

  • This motivated the parametric study of Pascoe et al (2019) to produce a seismological technique based on the results of numerical simulations which is not restricted by the thin boundary approximation

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Summary

Introduction

One of the key features which makes the plasma of the solar corona different from other natural plasma environments, for example, the Earth’s magnetosphere, is a pronounced fieldaligned filamentation of the macroscopic parameters, such as the density and temperature. Nakariakov, Dipankar Banerjee, Bo Li, Tongjiang Wang, Ivan Zimovets and Maurizio Falanga

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Empirical Properties of Decaying Kink Oscillations
Spectroscopic Observations of Kink Oscillations of Coronal Loops
The Zaitsev–Stepanov–Edwin–Roberts Model
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Damping of Kink Oscillations by Resonant Absorption
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Non-exponential Damping Regime of Resonant Absorption
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Kink Oscillations in Twisted Cylinders
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Kink Modes in the Presence of Parallel Shear Plasma Flows
Basic Effect of Flow on the Kink Eigen Frequency and Eigen Function
Kink Waves in Jets and Siphon Flows
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Negative Energy Wave Effects on Kink Oscillations
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Kink Oscillations in Loops Undergoing Cooling
Theoretical Modelling of the Period Ratio
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Effect of Perpendicular Nonuniformity
Effect of Axial Non-uniformity
Effect of Stationary Axial Flow
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10 Nonlinear Effects in Kink Oscillations
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10.2 Nonlinear Coupling of Kink and Fluting Oscillations
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10.3 Field-Aligned Flows Driven by the Ponderomotive Force in Kink Waves
11 Excitation of Kink Oscillations
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12 Decayless Kink Oscillations
12.1 Observations of Decayless Oscillations
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12.2 Theoretical and Numerical Models for Decayless Oscillations
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13 Possible Detection of Kink Oscillations in the Microwave and Radio Bands
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14 Conclusions and Outstanding Problems
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Findings
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Full Text
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