coronal bright points
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Solar Physics ◽  
2021 ◽  
Vol 296 (9) ◽  
Author(s):  
Rens van der Zwaard ◽  
Matthias Bergmann ◽  
Joe Zender ◽  
Rangaiah Kariyappa ◽  
Gabriel Giono ◽  
...  

AbstractThe study of solar irradiance variability is of great importance in heliophysics, Earth’s climate, and space weather applications. These studies require careful identifying, tracking and monitoring of features in the solar photosphere, chromosphere, and corona. Do coronal bright points contribute to the solar irradiance or its variability as input to the Earth atmosphere? We studied the variability of solar irradiance for a period of 10 years (May 2010 – June 2020) using the Large Yield Radiometer (LYRA), the Sun Watcher using APS and image Processing (SWAP) on board PROBA2, and the Atmospheric Imaging Assembly (AIA), and applied a linear model between the segmented features identified in the EUV images and the solar irradiance measured by LYRA. Based on EUV images from AIA, a spatial possibilistic clustering algorithm (SPoCA) is applied to identify coronal holes (CHs), and a morphological feature detection algorithm is applied to identify active regions (ARs), coronal bright points (BPs), and the quiet Sun (QS). The resulting segmentation maps were then applied on SWAP images, images of all AIA wavelengths, and parameters such as the intensity, fractional area, and contribution of ARs/CHs/BPs/QS features were computed and compared with LYRA irradiance measurements as a proxy for ultraviolet irradiation incident to the Earth atmosphere. We modeled the relation between the solar disk features (ARs, CHs, BPs, and QS) applied to EUV images against the solar irradiance as measured by LYRA and the F10.7 radio flux. A straightforward linear model was used and corresponding coefficients computed using a Bayesian method, indicating a strong influence of active regions to the EUV irradiance as measured at Earth’s atmosphere. It is concluded that the long- and short-term fluctuations of the active regions drive the EUV signal as measured at Earth’s atmosphere. A significant contribution from the bright points to the LYRA irradiance could not be found.


2021 ◽  
Vol 906 (1) ◽  
pp. 59
Author(s):  
Somaye Hosseini Rad ◽  
Nasibe Alipour ◽  
Hossein Safari

Author(s):  
Maria S. Madjarska ◽  
Jongchul Chae ◽  
Fernando Moreno-Insertis ◽  
Zhenyong Hou ◽  
Daniel Nobrega-Siverio ◽  
...  

Astrophysics ◽  
2020 ◽  
Vol 63 (3) ◽  
pp. 430-439
Author(s):  
T. Tsinamdzgvrishvili ◽  
B. Shergelashvili ◽  
B. Chargeishvili ◽  
I. Mghebrishvili ◽  
T. Mdzinarishvili ◽  
...  

2020 ◽  
Vol 893 (1) ◽  
pp. 64
Author(s):  
Léa Griton ◽  
Rui F. Pinto ◽  
Nicolas Poirier ◽  
Athanasios Kouloumvakos ◽  
Michäel Lavarra ◽  
...  

2019 ◽  
Vol 877 (2) ◽  
pp. 142 ◽  
Author(s):  
I. Skokić ◽  
R. Brajša ◽  
D. Sudar ◽  
D. Ruždjak ◽  
S. H. Saar

2019 ◽  
Vol 16 (1) ◽  
Author(s):  
Maria S. Madjarska

2019 ◽  
Vol 623 ◽  
pp. A78 ◽  
Author(s):  
Klaus Galsgaard ◽  
Maria S. Madjarska ◽  
Duncan H. Mackay ◽  
Chaozhou Mou

Context. Our recent observational study shows that the majority of coronal bright points (CBPs) in the quiet Sun are sources of one or more eruptions during their lifetime. Aims. Here, we investigate the non-potential time-dependent structure of the magnetic field of the CBP regions with special emphasis on the time-evolving magnetic structure at the spatial locations where the eruptions are initiated. Methods. The magnetic structure is evolved in time using a non-linear force-free field (NLFFF) relaxation approach based on a time series of helioseismic and magnetic imager (HMI) longitudinal magnetograms. This results in a continuous time series of NLFFFs. The time series is initiated with a potential field extrapolation based on a magnetogram taken well before the time of the eruptions. This initial field is then evolved in time in response to the observed changes in the magnetic field distribution at the photosphere. The local and global magnetic field structures from the time series of NLFFF field solutions are analysed in the vicinity of the eruption sites at the approximate times of the eruptions. Results. The analysis shows that many of the CBP eruptions reported in a recent publication contain a twisted flux tube located at the sites of eruptions. The presence of flux ropes at these locations provides in many cases a direct link between the magnetic field structure, their eruption, and the observation of mini coronal mass ejections (mini-CMEs). It is found that all repetitive eruptions are homologous. Conclusions. The NLFFF simulations show that twisted magnetic field structures are created at the locations hosting eruptions in CBPs. These twisted structures are produced by footpoint motions imposed by changes in the photospheric magnetic field observations. The true nature of the micro-flares remains unknown. Further 3D data-driven magnetohydrodynamic modelling is required to show how these twisted regions become unstable and erupt.


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