2016
DOI: 10.1002/9781119055006.ch25
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MHD Wave Modes Resolved in Fine‐Scale Chromospheric Magnetic Structures

Abstract: Within the last decade, due to significant improvements in the spatial and temporal resolution of chromospheric data, magnetohydrodynamic (MHD) wave studies in this fascinating region of the Sun's atmosphere have risen to the forefront of solar physics research. In this Chapter we begin by reviewing the challenges and debates that have manifested in relation to MHD wave mode identification in finescale chromospheric magnetic structures, including spicules, fibrils and mottles. Next we go on to discuss how the … Show more

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Cited by 27 publications
(13 citation statements)
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“…It is also unclear how to explain the observed periodicity if it is produced by Alfvén waves, as there have not been detections of coronal or chromospheric Alfvén waves with the detected periodicity (see e.g. Jess et al 2015;Verth & Jess 2016).…”
Section: Physical Mechanismmentioning
confidence: 99%
“…It is also unclear how to explain the observed periodicity if it is produced by Alfvén waves, as there have not been detections of coronal or chromospheric Alfvén waves with the detected periodicity (see e.g. Jess et al 2015;Verth & Jess 2016).…”
Section: Physical Mechanismmentioning
confidence: 99%
“…Notably, compressible and incompressible MHD-wave modes can be excited in magnetic flux tubes, which act as waveguides, by reoccurring perturbations at their footpoints at photospheric heights [7]. Signatures of both standing and propagating incompressible (transverse) kink waves, as oscillatory pattern of velocities perpendicular to the assumed waveguides, have been observed in various structures in the solar photosphere and chromosphere such as small-scale bright points, spicules, fibrils, and mottles (e.g., [8][9][10][11][12][13][14][15][16]).…”
Section: Introductionmentioning
confidence: 99%
“…(2009) measured the amplitude of H α non‐thermal line broadening to be ∼0.05 Å (or a velocity amplitude on the order of 2.5 km s −1 ; upper‐right panel of Figure 4), and when combined with a plasma density of ∼10 −9 g cm −3 and a local Alfvén speed of ∼22 km s −1 , provided a wave energy flux equal to ∼150,000 W m −2 . While this quantity of energy is far in excess of the amount required to balance chromospheric radiative losses (Withbroe & Noyes, 1977), Verth and Jess (2016) hypothesized that the filling factor of such waves needs to be evaluated before the true importance of their existence can be evaluated. With this in mind, Fedun, Verth, et al.…”
Section: Waves In Structured Flux Tubes In the Chromospherementioning
confidence: 99%