A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734

We present a detailed analysis of a partial eruption of a sigmoid filament lying along the polarity inversion line (PIL) of the small active region (AR) NOAA 12734 (with an area of 1.44 <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline">...

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Main Authors: Jihong Liu, Yin Zhang, Yuhong Zheng, Yu Liu, Jie Chen
Format: Article
Language:English
Published: MDPI AG 2024-01-01
Series:Universe
Subjects:
Online Access:https://www.mdpi.com/2218-1997/10/1/42
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author Jihong Liu
Yin Zhang
Yuhong Zheng
Yu Liu
Jie Chen
author_facet Jihong Liu
Yin Zhang
Yuhong Zheng
Yu Liu
Jie Chen
author_sort Jihong Liu
collection DOAJ
description We present a detailed analysis of a partial eruption of a sigmoid filament lying along the polarity inversion line (PIL) of the small active region (AR) NOAA 12734 (with an area of 1.44 <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo>×</mo><mspace width="3.33333pt"></mspace><msup><mn>10</mn><mn>3</mn></msup></mrow></semantics></math></inline-formula> square megameters). The active filament was rooted in a dipole sunspot of the AR. The eruption was associated with a C1.3 flare and subsequent large-scale coronal disturbances. During its solar disk passage before the flare, the AR had the following characteristics: (1) Most of the time, the magnetic field lines in the AR showed a sigmoidal structure (‘L1’) in the low corona and arc-shaped loops (i.e., ‘L2’) in the upper atmosphere. (2) An ‘X’-shaped structure was formed between the original ‘S’-shaped magnetic loop (‘L1’) and the newly rising one (‘L3’) between the main positive and negative magnetic polarities of the sunspots, and the intersection point of flux ropes ‘L1’ and ‘L3’ corresponds well with the area where the initial extreme-ultraviolet (EUV) 1600 Å brightening of the flare occurred. (3) The AR disobeyed the hemispherical helicity rule and had magnetic twist and writhe of the same signs, i.e., its magnetic helicity/current helicity were positive in the northern hemisphere. (4) Sustained magnetic emergence and cancellation occurred before the flare. Therefore, the magnetic reconnection of highly twisted helical flux ropes under the confinement of the overlying magnetic fields is probably responsible for the partial eruption of the filament.
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spelling doaj.art-50fdb98e94b6431c8faf6330843647ca2024-01-26T18:43:06ZengMDPI AGUniverse2218-19972024-01-011014210.3390/universe10010042A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734Jihong Liu0Yin Zhang1Yuhong Zheng2Yu Liu3Jie Chen4School of Science, Shijiazhuang University, Shijiazhuang 050035, ChinaNational Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012, ChinaShijiazhuang Post and Telecommunications Technical College, Shijiazhuang 050011, ChinaSchool of Physical Science and Technology, Southwest Jiaotong University, Chengdu 610031, ChinaNational Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012, ChinaWe present a detailed analysis of a partial eruption of a sigmoid filament lying along the polarity inversion line (PIL) of the small active region (AR) NOAA 12734 (with an area of 1.44 <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mo>×</mo><mspace width="3.33333pt"></mspace><msup><mn>10</mn><mn>3</mn></msup></mrow></semantics></math></inline-formula> square megameters). The active filament was rooted in a dipole sunspot of the AR. The eruption was associated with a C1.3 flare and subsequent large-scale coronal disturbances. During its solar disk passage before the flare, the AR had the following characteristics: (1) Most of the time, the magnetic field lines in the AR showed a sigmoidal structure (‘L1’) in the low corona and arc-shaped loops (i.e., ‘L2’) in the upper atmosphere. (2) An ‘X’-shaped structure was formed between the original ‘S’-shaped magnetic loop (‘L1’) and the newly rising one (‘L3’) between the main positive and negative magnetic polarities of the sunspots, and the intersection point of flux ropes ‘L1’ and ‘L3’ corresponds well with the area where the initial extreme-ultraviolet (EUV) 1600 Å brightening of the flare occurred. (3) The AR disobeyed the hemispherical helicity rule and had magnetic twist and writhe of the same signs, i.e., its magnetic helicity/current helicity were positive in the northern hemisphere. (4) Sustained magnetic emergence and cancellation occurred before the flare. Therefore, the magnetic reconnection of highly twisted helical flux ropes under the confinement of the overlying magnetic fields is probably responsible for the partial eruption of the filament.https://www.mdpi.com/2218-1997/10/1/42flaresfilaments/prominencesmagnetic fieldsreconnection
spellingShingle Jihong Liu
Yin Zhang
Yuhong Zheng
Yu Liu
Jie Chen
A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734
Universe
flares
filaments/prominences
magnetic fields
reconnection
title A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734
title_full A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734
title_fullStr A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734
title_full_unstemmed A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734
title_short A Partial Eruption of a Sigmoid Filament in the Small Dipole Active Region 12734
title_sort partial eruption of a sigmoid filament in the small dipole active region 12734
topic flares
filaments/prominences
magnetic fields
reconnection
url https://www.mdpi.com/2218-1997/10/1/42
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