{"title":"不同耀斑生产率水平下活动区纵向磁场的横向梯度。II.统计分析","authors":"Yu. A. Fursyak","doi":"10.1007/s10511-024-09818-1","DOIUrl":null,"url":null,"abstract":"<p>Here, we performed a statistical analysis of the parameters describing the transverse component of the longitudinal magnetic field gradient (∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> ) in the active regions of the AR – the AR-averaged transverse component of the longitudinal magnetic field gradient <∇ <sub>⊥</sub> <b><i>B z</i></b> >, the average transverse component of the longitudinal magnetic field gradient in the vicinity of a point with its maximum value <max∇ <sub>⊥</sub> <b><i>B z</i></b> >, the maximum value of the transverse component of the longitudinal magnetic field gradient between pairs of spots in the AR max(∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> ) <sub><i>sp</i></sub> . For calculating the denoted parameters, magnetograms of the <b><i>B</i></b> <sub>z</sub> -components of the magnetic field vector at the level of the Sun’s photosphere obtained by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO) are used. The statistical sample contains data on 75 ARs. The values of the analyzed parameters obtained over the time of monitoring are compared with the level of flare productivity of the AR (the flare index FI). It is shown that: 1. The <span>\\(\\langle \\overline{{\\nabla }_{\\perp }{{\\varvec{B}}}_{z}}\\rangle \\)</span> -FI dependence (the overhead line denotes averaging over the time of monitoring the AR) is quadratic with a correlation coefficient k = 0.54 while the spread in values of the quantity <span>\\(\\langle \\overline{{\\nabla }_{\\perp }{{\\varvec{B}}}_{z}}\\rangle \\)</span> is small (lying within a a range of 0.08-0.12 G km<sup>-1</sup> for the overwhelming majority of the studied regions) and differs very little for regions with low and high flare productivity, which may be explained by the dependence of ∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> on the area of the AR. 2. The dependence <span>\\(\\langle \\overline{{\\text{max}}{\\nabla }_{\\perp }{{\\varvec{B}}}_{z}}\\rangle \\)</span> -FI is quasilinear with a correlation coefficient k = 0.61. 3. The dependence <span>\\(\\overline{{\\text{max}}{\\nabla }_{\\perp }{{\\varvec{B}}}_{z}}\\)</span> -FI is linear with a correlation coefficient k = 0.63. 4. The threshold values of the analyzed parameters are found: for <span>\\(\\langle \\overline{{\\nabla }_{\\perp }{{\\varvec{B}}}_{z}}\\rangle \\)</span> ≥ 0.078 G km<sup>-1</sup>, for <span>\\(\\langle \\overline{{\\text{max}}{\\nabla }_{\\perp }{{\\varvec{B}}}_{z}}\\rangle \\)</span> ≥ 0.983 G km<sup>-1</sup>, and for the parameter max(∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub>) <sub><i>sp</i></sub> ≥ 0.118G km<sup>-1</sup>. For lower values of the analyzed parameters, no x-ray flares were recorded in any of the ARs of the analyzed sample.</p>","PeriodicalId":479,"journal":{"name":"Astrophysics","volume":null,"pages":null},"PeriodicalIF":0.6000,"publicationDate":"2024-05-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Transverse Gradients of Longitudinal Magnetic Field in Active Regions with Different Levels of Flare Productivity. II. Statistical Analysis\",\"authors\":\"Yu. A. Fursyak\",\"doi\":\"10.1007/s10511-024-09818-1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Here, we performed a statistical analysis of the parameters describing the transverse component of the longitudinal magnetic field gradient (∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> ) in the active regions of the AR – the AR-averaged transverse component of the longitudinal magnetic field gradient <∇ <sub>⊥</sub> <b><i>B z</i></b> >, the average transverse component of the longitudinal magnetic field gradient in the vicinity of a point with its maximum value <max∇ <sub>⊥</sub> <b><i>B z</i></b> >, the maximum value of the transverse component of the longitudinal magnetic field gradient between pairs of spots in the AR max(∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> ) <sub><i>sp</i></sub> . For calculating the denoted parameters, magnetograms of the <b><i>B</i></b> <sub>z</sub> -components of the magnetic field vector at the level of the Sun’s photosphere obtained by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO) are used. The statistical sample contains data on 75 ARs. The values of the analyzed parameters obtained over the time of monitoring are compared with the level of flare productivity of the AR (the flare index FI). It is shown that: 1. The <span>\\\\(\\\\langle \\\\overline{{\\\\nabla }_{\\\\perp }{{\\\\varvec{B}}}_{z}}\\\\rangle \\\\)</span> -FI dependence (the overhead line denotes averaging over the time of monitoring the AR) is quadratic with a correlation coefficient k = 0.54 while the spread in values of the quantity <span>\\\\(\\\\langle \\\\overline{{\\\\nabla }_{\\\\perp }{{\\\\varvec{B}}}_{z}}\\\\rangle \\\\)</span> is small (lying within a a range of 0.08-0.12 G km<sup>-1</sup> for the overwhelming majority of the studied regions) and differs very little for regions with low and high flare productivity, which may be explained by the dependence of ∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub> on the area of the AR. 2. The dependence <span>\\\\(\\\\langle \\\\overline{{\\\\text{max}}{\\\\nabla }_{\\\\perp }{{\\\\varvec{B}}}_{z}}\\\\rangle \\\\)</span> -FI is quasilinear with a correlation coefficient k = 0.61. 3. The dependence <span>\\\\(\\\\overline{{\\\\text{max}}{\\\\nabla }_{\\\\perp }{{\\\\varvec{B}}}_{z}}\\\\)</span> -FI is linear with a correlation coefficient k = 0.63. 4. The threshold values of the analyzed parameters are found: for <span>\\\\(\\\\langle \\\\overline{{\\\\nabla }_{\\\\perp }{{\\\\varvec{B}}}_{z}}\\\\rangle \\\\)</span> ≥ 0.078 G km<sup>-1</sup>, for <span>\\\\(\\\\langle \\\\overline{{\\\\text{max}}{\\\\nabla }_{\\\\perp }{{\\\\varvec{B}}}_{z}}\\\\rangle \\\\)</span> ≥ 0.983 G km<sup>-1</sup>, and for the parameter max(∇ <sub>⊥</sub> <b><i>B </i></b><sub><i>z</i></sub>) <sub><i>sp</i></sub> ≥ 0.118G km<sup>-1</sup>. For lower values of the analyzed parameters, no x-ray flares were recorded in any of the ARs of the analyzed sample.</p>\",\"PeriodicalId\":479,\"journal\":{\"name\":\"Astrophysics\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.6000,\"publicationDate\":\"2024-05-17\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Astrophysics\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s10511-024-09818-1\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"ASTRONOMY & ASTROPHYSICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Astrophysics","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1007/s10511-024-09818-1","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"ASTRONOMY & ASTROPHYSICS","Score":null,"Total":0}
引用次数: 0
摘要
最大值点附近纵向磁场梯度的平均横向分量 <max∇⊥B z >,AR max(∇ ⊥B z ) sp 中点对点之间纵向磁场梯度横向分量的最大值。为了计算所标注的参数,使用了太阳动力学观测台(SDO)上的太阳地震和磁场成像仪(HMI)获得的太阳光层水平磁场矢量 B z 分量的磁图。统计样本包含 75 个 AR 的数据。将监测期间获得的分析参数值与 AR 的耀斑生产力水平(耀斑指数 FI)进行了比较。结果表明1.(\langle \overline{{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \)-FI相关性(架空线表示在监测AR的时间内的平均值)是二次的,相关系数k = 0.54 而 \(\langle \overline{{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \)量值的差值很小(在 0.08-0.12 G km-1 的范围内),而且在耀斑生产率低和高的地区差别很小,这可以用 ∇ ⊥ B z 与 AR 面积的关系来解释。2.依赖关系((\langle \overline{{text{max}}{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \)-FI 是准线性关系,相关系数 k = 0.61。3.依赖关系 \(\overline{\{text{max}}{\nabla }_{\perp }{{{varvec{B}}}_{z}}\) -FI 是线性的,相关系数 k = 0.63。4.找到了分析参数的临界值:对于 \(angle \overline{{\nabla }_{per\p }{{\varvec{B}}}_{z}}\rangle \) ≥ 0.078 G km-1, for \(\langle overline{{text{max}}{\nabla }_{\perp }{{{varvec{B}}}_{z}}\rangle \) ≥ 0.983 G km-1, and for the parameter max(∇ ⊥ B z) sp ≥ 0.118G km-1.对于较低的分析参数值,分析样本中的任何一个AR都没有记录到X射线耀斑。
Transverse Gradients of Longitudinal Magnetic Field in Active Regions with Different Levels of Flare Productivity. II. Statistical Analysis
Here, we performed a statistical analysis of the parameters describing the transverse component of the longitudinal magnetic field gradient (∇ ⊥B z ) in the active regions of the AR – the AR-averaged transverse component of the longitudinal magnetic field gradient <∇ ⊥B z >, the average transverse component of the longitudinal magnetic field gradient in the vicinity of a point with its maximum value <max∇ ⊥B z >, the maximum value of the transverse component of the longitudinal magnetic field gradient between pairs of spots in the AR max(∇ ⊥B z ) sp . For calculating the denoted parameters, magnetograms of the Bz -components of the magnetic field vector at the level of the Sun’s photosphere obtained by the Helioseismic and Magnetic Imager (HMI) on board the Solar Dynamics Observatory (SDO) are used. The statistical sample contains data on 75 ARs. The values of the analyzed parameters obtained over the time of monitoring are compared with the level of flare productivity of the AR (the flare index FI). It is shown that: 1. The \(\langle \overline{{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \) -FI dependence (the overhead line denotes averaging over the time of monitoring the AR) is quadratic with a correlation coefficient k = 0.54 while the spread in values of the quantity \(\langle \overline{{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \) is small (lying within a a range of 0.08-0.12 G km-1 for the overwhelming majority of the studied regions) and differs very little for regions with low and high flare productivity, which may be explained by the dependence of ∇ ⊥B z on the area of the AR. 2. The dependence \(\langle \overline{{\text{max}}{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \) -FI is quasilinear with a correlation coefficient k = 0.61. 3. The dependence \(\overline{{\text{max}}{\nabla }_{\perp }{{\varvec{B}}}_{z}}\) -FI is linear with a correlation coefficient k = 0.63. 4. The threshold values of the analyzed parameters are found: for \(\langle \overline{{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \) ≥ 0.078 G km-1, for \(\langle \overline{{\text{max}}{\nabla }_{\perp }{{\varvec{B}}}_{z}}\rangle \) ≥ 0.983 G km-1, and for the parameter max(∇ ⊥B z) sp ≥ 0.118G km-1. For lower values of the analyzed parameters, no x-ray flares were recorded in any of the ARs of the analyzed sample.
期刊介绍:
Astrophysics (Ap) is a peer-reviewed scientific journal which publishes research in theoretical and observational astrophysics. Founded by V.A.Ambartsumian in 1965 Astrophysics is one of the international astronomy journals. The journal covers space astrophysics, stellar and galactic evolution, solar physics, stellar and planetary atmospheres, interstellar matter. Additional subjects include chemical composition and internal structure of stars, quasars and pulsars, developments in modern cosmology and radiative transfer.