Pub Date : 2024-09-20DOI: 10.1007/s11207-024-02377-w
Werner Däppen
A controversy about the possibility of dynamic effects in nuclear screening has been around for several decades. On the one hand, there is the claim that there are no dynamic effects and that the classic Salpeter correction based on static Debye screening is all that is needed for astrophysical applications. The size of the correction is on the order of 5% in typical solar fusion reactions. On the other hand, numerical simulations have shown that there is a dynamical effect, which essentially cancels the Salpeter correction. The results of the numerical simulations were later independently confirmed. The astrophysical community, however, has so far largely ignored the possibility of dynamical screening. The present paper is meant to serve as a reminder of the controversy. Not only does the claim of an absence of a dynamical effect equally warrant an independent confirmation, but there is motivation for further investigation, such as the assessment of current laboratory experiments and a quantitative study of the dynamical effect in case it will turn out to be real.
{"title":"The Current State of the Controversy over Screening in Nuclear Reactions","authors":"Werner Däppen","doi":"10.1007/s11207-024-02377-w","DOIUrl":"10.1007/s11207-024-02377-w","url":null,"abstract":"<div><p>A controversy about the possibility of dynamic effects in nuclear screening has been around for several decades. On the one hand, there is the claim that there are no dynamic effects and that the classic Salpeter correction based on static Debye screening is all that is needed for astrophysical applications. The size of the correction is on the order of 5% in typical solar fusion reactions. On the other hand, numerical simulations have shown that there is a dynamical effect, which essentially cancels the Salpeter correction. The results of the numerical simulations were later independently confirmed. The astrophysical community, however, has so far largely ignored the possibility of dynamical screening. The present paper is meant to serve as a reminder of the controversy. Not only does the claim of an absence of a dynamical effect equally warrant an independent confirmation, but there is motivation for further investigation, such as the assessment of current laboratory experiments and a quantitative study of the dynamical effect in case it will turn out to be real.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142412774","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-20DOI: 10.1007/s11207-024-02375-y
Avneesh Kumar, Nagendra Kumar, Hari Om Vats
We study the temporal variation of solar rotation profiles based on solar irradiance at 93.5 nm and solar radio flux at 10.7 cm originating from the transition region and lower corona, respectively. The autocorrelation technique is used to calculate the period in periodic time series data. The sidereal rotation periods for normalized and detrended data are studied for 2011 – 2021. The sidereal rotation periods for solar irradiance and radio flux for 2011 – 2021 vary from 22.75 to 26.17 days and 19.42 to 28.14 days, respectively. The mean of the sidereal rotation periods for solar irradiance and radio flux are 24.76 and 23.76 days, respectively. The mean sidereal rotation period for solar irradiance is higher than the mean sidereal rotation period for solar radio flux. The sidereal rotation period for solar irradiance is greater than or equal to the sidereal rotation period for solar radio flux for almost all the years between 2011 and 2021. It is found that the lower corona rotates faster than the transition region during 2011 – 2021, i.e., the lower corona is found to be moving 4% faster than the transition region during 2011 – 2021. We found a linear relationship between the normalized daily irradiance and radio flux with a correlation coefficient of 0.986. Using cross-correlation analysis, we investigated a phase relationship between solar irradiance and radio flux and found no time lag between solar irradiance and radio flux.
{"title":"Comparative Study of Solar Rotation of Transition Region and Corona using Solar Irradiance and Radio Flux","authors":"Avneesh Kumar, Nagendra Kumar, Hari Om Vats","doi":"10.1007/s11207-024-02375-y","DOIUrl":"10.1007/s11207-024-02375-y","url":null,"abstract":"<div><p>We study the temporal variation of solar rotation profiles based on solar irradiance at 93.5 nm and solar radio flux at 10.7 cm originating from the transition region and lower corona, respectively. The autocorrelation technique is used to calculate the period in periodic time series data. The sidereal rotation periods for normalized and detrended data are studied for 2011 – 2021. The sidereal rotation periods for solar irradiance and radio flux for 2011 – 2021 vary from 22.75 to 26.17 days and 19.42 to 28.14 days, respectively. The mean of the sidereal rotation periods for solar irradiance and radio flux are 24.76 and 23.76 days, respectively. The mean sidereal rotation period for solar irradiance is higher than the mean sidereal rotation period for solar radio flux. The sidereal rotation period for solar irradiance is greater than or equal to the sidereal rotation period for solar radio flux for almost all the years between 2011 and 2021. It is found that the lower corona rotates faster than the transition region during 2011 – 2021, i.e., the lower corona is found to be moving 4% faster than the transition region during 2011 – 2021. We found a linear relationship between the normalized daily irradiance and radio flux with a correlation coefficient of 0.986. Using cross-correlation analysis, we investigated a phase relationship between solar irradiance and radio flux and found no time lag between solar irradiance and radio flux.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142412811","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-20DOI: 10.1007/s11207-024-02373-0
V. V. Grechnev, V. I. Kiselev, A. M. Uralov, N. S. Meshalkina, K. A. Firoz, A. L. Lysenko
The SOL2012-05-17 event is remarkable in that it caused one of two ground-level enhancements (GLE71) in Solar Cycle 24. Despite the efforts spent studying this solar event, some aspects of it remain unclear. This relates to the development of a coronal mass ejection (CME), the history of the shock wave, and the flare. Our measurements reveal the following chain of phenomena. Two successive eruptions occurred within a few minutes. The rate of change of the reconnected magnetic flux shows a series of increases corresponding to the acceleration or deceleration of the erupting structures. The temporal profile of the magnetic-flux change rate is similar to the hard X-ray burst. Each eruption excited a disturbance that, propagating outward, accelerated all structures above it. This led to complex kinematic characteristics of the erupting structures that eventually formed a self-similarly expanding CME. The two disturbances became piston shocks and merged into a single, stronger shock. There are indications of transformation of the piston shock into a bow shock, but this occurs at distances exceeding ten solar radii. Components of the described picture were observed in a number of events and can serve as a guide for studies of eruptive flares.
SOL2012-05-17 太阳活动是太阳活动周期 24 中两次地面增强(GLE71)中的一次。尽管对这一太阳活动进行了大量研究,但它的某些方面仍不清楚。这与日冕物质抛射(CME)的发展、冲击波的历史和耀斑有关。我们的测量结果揭示了以下一系列现象。几分钟内连续发生了两次爆发。重新连接的磁通量的变化率显示出一系列与爆发结构的加速或减速相对应的增长。磁通量变化率的时间曲线与硬 X 射线爆发相似。每次爆发都会激发一个扰动,该扰动向外传播,加速了其上方的所有结构。这导致喷发结构具有复杂的运动特性,最终形成一个自相似膨胀的 CME。这两个扰动变成了活塞冲击,并合并成一个更强的冲击。有迹象表明活塞冲击转变为弓形冲击,但这发生在距离超过 10 个太阳半径的地方。在一些事件中观测到了所述图景的组成部分,可作为爆发耀斑研究的指南。
{"title":"Mysteries of the 17 May 2012 Solar Event Responsible for GLE71. I. CME Development and the Role of Disturbances Excited by Eruptions","authors":"V. V. Grechnev, V. I. Kiselev, A. M. Uralov, N. S. Meshalkina, K. A. Firoz, A. L. Lysenko","doi":"10.1007/s11207-024-02373-0","DOIUrl":"10.1007/s11207-024-02373-0","url":null,"abstract":"<div><p>The SOL2012-05-17 event is remarkable in that it caused one of two ground-level enhancements (GLE71) in Solar Cycle 24. Despite the efforts spent studying this solar event, some aspects of it remain unclear. This relates to the development of a coronal mass ejection (CME), the history of the shock wave, and the flare. Our measurements reveal the following chain of phenomena. Two successive eruptions occurred within a few minutes. The rate of change of the reconnected magnetic flux shows a series of increases corresponding to the acceleration or deceleration of the erupting structures. The temporal profile of the magnetic-flux change rate is similar to the hard X-ray burst. Each eruption excited a disturbance that, propagating outward, accelerated all structures above it. This led to complex kinematic characteristics of the erupting structures that eventually formed a self-similarly expanding CME. The two disturbances became piston shocks and merged into a single, stronger shock. There are indications of transformation of the piston shock into a bow shock, but this occurs at distances exceeding ten solar radii. Components of the described picture were observed in a number of events and can serve as a guide for studies of eruptive flares.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142412683","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-20DOI: 10.1007/s11207-024-02350-7
A. Posner, I. G. Richardson, R. D.-T. Strauss
This work analyzes the appearance of wide-spread deka-MeV solar energetic proton (SEP) events, in particular the arrival of the first protons within ≈ 4.5 – 45 MeV measured at Earth–Sun L1, and their relationship with their relative solar source longitude. The definition of “wide-spread SEP event” for this study refers to events that are observed as a 25 MeV proton intensity increase at near 1 AU locations that are separated by at least 130∘ in solar longitude. Many of these events are seen at all three of the spacecraft, STEREO (Solar-Terrestrial Relations Observatory) A, STEREO B, and SOHO (Solar and Heliospheric Observatory), and may therefore extend far beyond 130∘ in longitude around the Sun. A large subset of these events have already been part of a study by Richardson et al. (Solar Phys., 289, 3059, 2014). The event source region identifications draw from this study; more recent events have also been added. Our focus is on answering two specific questions: (1) What is the maximum longitude over which SEP protons show energy dispersion, i.e., a clear sign of arrival of higher-energy protons before those of lower energy? (2) What implications can be drawn from the ensemble of events observed regarding either direct magnetic connectivity to shocks and/or cross-field transport from the site of the eruption in the onset phase of the event?
{"title":"The “SEP Clock”: A Discussion of First Proton Arrival Times in Wide-Spread Solar Energetic Particle Events","authors":"A. Posner, I. G. Richardson, R. D.-T. Strauss","doi":"10.1007/s11207-024-02350-7","DOIUrl":"10.1007/s11207-024-02350-7","url":null,"abstract":"<div><p>This work analyzes the appearance of wide-spread deka-MeV solar energetic proton (SEP) events, in particular the arrival of the first protons within ≈ 4.5 – 45 MeV measured at Earth–Sun L1, and their relationship with their relative solar source longitude. The definition of “wide-spread SEP event” for this study refers to events that are observed as a 25 MeV proton intensity increase at near 1 AU locations that are separated by at least 130<sup>∘</sup> in solar longitude. Many of these events are seen at all three of the spacecraft, STEREO (Solar-Terrestrial Relations Observatory) A, STEREO B, and SOHO (Solar and Heliospheric Observatory), and may therefore extend far beyond 130<sup>∘</sup> in longitude around the Sun. A large subset of these events have already been part of a study by Richardson et al. (<i>Solar Phys</i>., <b>289</b>, 3059, 2014). The event source region identifications draw from this study; more recent events have also been added. Our focus is on answering two specific questions: (1) What is the maximum longitude over which SEP protons show energy dispersion, i.e., a clear sign of arrival of higher-energy protons before those of lower energy? (2) What implications can be drawn from the ensemble of events observed regarding either direct magnetic connectivity to shocks and/or cross-field transport from the site of the eruption in the onset phase of the event?</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s11207-024-02350-7.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142412773","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-19DOI: 10.1007/s11207-024-02351-6
Tsvetan Tsvetkov, Yoana Nakeva, Nikola Petrov
We present a statistical study on the relationship of solar dynamic events (solar flares and coronal mass ejections) with active regions during Solar Cycle 24 (December 2008–December 2019). Combining data from NOAA Space Weather Prediction Center and observations of Large Angle and Spectrometric Coronagraph (LASCO) onboard the Solar and Heliospheric Observatory (SOHO) spacecraft, we found that more than a half of the coronal mass ejections were generated inside active regions. Geostationary Operational Environmental Satellite (GOES) soft X-ray flare listing data completed our study showing that almost 83% of Solar Cycle 24 flares are connected with active regions. Finally, we summarize the details for the related phenomena into an online catalog based on a list of all 1533 active regions that produced at least one flare and/or coronal mass ejection during Solar Cycle 24 and explore their properties like flare class, coronal mass ejection speed, and angular width paying special attention to the most powerful and threatful to Earth solar events.
我们介绍了太阳动力学事件(太阳耀斑和日冕物质抛射)与太阳周期24(2008年12月至2019年12月)期间活动区域关系的统计研究。结合美国国家海洋和大气管理局(NOAA)空间天气预报中心的数据以及太阳和日光层观测站(SOHO)航天器上的大角度和分光日冕仪(LASCO)的观测数据,我们发现超过一半的日冕物质抛射是在活动区域内产生的。地球静止业务环境卫星(GOES)的软 X 射线耀斑列表数据完成了我们的研究,显示太阳周期 24 几乎 83% 的耀斑与活动区有关。最后,我们在太阳周期24期间至少产生过一次耀斑和/或日冕物质抛射的所有1533个活动区列表的基础上,将相关现象的详细信息汇总到一个在线目录中,并探讨了它们的特性,如耀斑等级、日冕物质抛射速度和角宽度,特别关注了最强大和对地球威胁最大的太阳活动。
{"title":"Online Catalog of Activity Events of Solar Cycle 24 Related to Active Regions","authors":"Tsvetan Tsvetkov, Yoana Nakeva, Nikola Petrov","doi":"10.1007/s11207-024-02351-6","DOIUrl":"10.1007/s11207-024-02351-6","url":null,"abstract":"<div><p>We present a statistical study on the relationship of solar dynamic events (solar flares and coronal mass ejections) with active regions during Solar Cycle 24 (December 2008–December 2019). Combining data from NOAA Space Weather Prediction Center and observations of Large Angle and Spectrometric Coronagraph (LASCO) onboard the Solar and Heliospheric Observatory (SOHO) spacecraft, we found that more than a half of the coronal mass ejections were generated inside active regions. Geostationary Operational Environmental Satellite (GOES) soft X-ray flare listing data completed our study showing that almost 83% of Solar Cycle 24 flares are connected with active regions. Finally, we summarize the details for the related phenomena into an online catalog based on a list of all 1533 active regions that produced at least one flare and/or coronal mass ejection during Solar Cycle 24 and explore their properties like flare class, coronal mass ejection speed, and angular width paying special attention to the most powerful and threatful to Earth solar events.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142412601","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-09DOI: 10.1007/s11207-024-02365-0
V. N. Obridko, M. M. Katsova, D. D. Sokoloff, N. V. Emelianov
This work continues our research of the connection between the long-term activity of stars and their planets. We analyze new data on the previously considered two dozen solar-type stars with identified cycles, adding the results of studying the long-term variability of two more solar-type G stars and 15 cooler M dwarfs with planets. If the cyclic activity is determined by a strong tidal influence of the planet, then the cycle duration of the star should be synchronized with the period of orbital revolution of the planet. We calculate the gravitational effect of planets on their parent stars. The results obtained confirm the earlier conclusion that exoplanets do not influence the formation of the stellar cycle. We examine the change in the position of the barycenter of the solar system relative to the center of the Sun over 420 years. A comparison of these data with the most reliable 120-year SSN (sunspot number) series as the index of solar activity has shown that they are not synchronized.
{"title":"Is There a Synchronizing Influence of Planets on Solar and Stellar Cyclic Activity?","authors":"V. N. Obridko, M. M. Katsova, D. D. Sokoloff, N. V. Emelianov","doi":"10.1007/s11207-024-02365-0","DOIUrl":"10.1007/s11207-024-02365-0","url":null,"abstract":"<div><p>This work continues our research of the connection between the long-term activity of stars and their planets. We analyze new data on the previously considered two dozen solar-type stars with identified cycles, adding the results of studying the long-term variability of two more solar-type G stars and 15 cooler M dwarfs with planets. If the cyclic activity is determined by a strong tidal influence of the planet, then the cycle duration of the star should be synchronized with the period of orbital revolution of the planet. We calculate the gravitational effect of planets on their parent stars. The results obtained confirm the earlier conclusion that exoplanets do not influence the formation of the stellar cycle. We examine the change in the position of the barycenter of the solar system relative to the center of the Sun over 420 years. A comparison of these data with the most reliable 120-year SSN (sunspot number) series as the index of solar activity has shown that they are not synchronized.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142219147","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-05DOI: 10.1007/s11207-024-02358-z
Ekaterina Dineva, Carsten Denker, Meetu Verma, Klaus Strassmeier, Ilya Ilyin, Ivan Milic
The solar eclipse of 2017 August 21 was observed with the Potsdam Echelle Polarimetric and Spectroscopic Instrument (PEPSI) on the Large Binocular Telescope (LBT), which is located at Mt. Graham International Observatory (MGIO), Arizona, USA. At this location, a partial eclipse was observed with maximum obscuration of about 61.6%. The 11-millimeter-aperture, binocular Solar Disk-Integrated (SDI) telescope, located on the kitchen balcony of the LBT building, feeds sunlight to PEPSI, which has recorded a total of 116 Sun-as-a-star spectra in the wavelength range of 5300 – 6300 Å, with a spectral resolution ({mathcal{R}} approx 250{,}000) and signal-to-noise ratio of about 733:1. The temporal evolution of the Fraunhofer Na i D doublet at (lambda )5890/5896 Å is analyzed using contrast profiles that illustrate subtle changes in the spectral line, not obvious in the intensity profiles. Line bisectors are used to study the height-dependent signature of convective motions. Sun-as-a-star spectra illustrate the radial atmospheric stratification and are affected by limb darkening, solar differential rotation, convective motions, and magnetic activity. During a partial solar eclipse, the contribution of these features is modified by the passage of the Moon, resulting in a transit spectral signature. These observations are compared with synthetic Na i D spectra generated by the Spectropolarimetic NLTE Analytically Powered Inversion (SNAPI) code, based on state-of-the-art Bifrost atmospheric parameters, applied to a geometrically accurate model of the solar eclipse. The model is in qualitative agreement with the observations. However, the discrepancies indicate that models need to be improved, where high-resolution eclipse spectroscopy can serve as a benchmark.
位于美国亚利桑那州格雷厄姆山国际天文台(MGIO)的大型双筒望远镜(LBT)上的波茨坦梯度偏振和光谱仪器(PEPSI)观测到了 2017 年 8 月 21 日的日食。在该地点观测到的偏食最大遮蔽率约为 61.6%。该望远镜记录了波长范围为 5300 - 6300 Å 的 116 条太阳恒星光谱,光谱分辨率({mathcal{R}} approx 250{,}000/)和信噪比(signal-to-noise ratio)约为 733:1。使用对比剖面图分析了 (lambda )5890/5896 Å 处弗劳恩霍夫 Na i D 双线的时间演变,该剖面图显示了光谱线的微妙变化,而在强度剖面图中并不明显。利用谱线二分线来研究对流运动随高度变化的特征。太阳恒星光谱显示了径向大气分层,并受到边缘变暗、太阳差转、对流运动和磁活动的影响。在日偏食期间,这些特征的贡献会因月球的通过而改变,从而产生过境光谱特征。这些观测数据与由光谱拟态 NLTE 分析驱动反演(SNAPI)代码生成的合成 Na i D 光谱进行了比较,SNAPI 代码基于最先进的 Bifrost 大气参数,应用于日食几何精确模型。该模型与观测结果在质量上是一致的。然而,差异表明模型需要改进,高分辨率日食光谱可作为基准。
{"title":"High-Resolution Sun-as-a-Star Spectroscopy of the Partial Solar Eclipse of 2017 August 21","authors":"Ekaterina Dineva, Carsten Denker, Meetu Verma, Klaus Strassmeier, Ilya Ilyin, Ivan Milic","doi":"10.1007/s11207-024-02358-z","DOIUrl":"10.1007/s11207-024-02358-z","url":null,"abstract":"<div><p>The solar eclipse of 2017 August 21 was observed with the Potsdam Echelle Polarimetric and Spectroscopic Instrument (PEPSI) on the Large Binocular Telescope (LBT), which is located at Mt. Graham International Observatory (MGIO), Arizona, USA. At this location, a partial eclipse was observed with maximum obscuration of about 61.6%. The 11-millimeter-aperture, binocular Solar Disk-Integrated (SDI) telescope, located on the kitchen balcony of the LBT building, feeds sunlight to PEPSI, which has recorded a total of 116 Sun-as-a-star spectra in the wavelength range of 5300 – 6300 Å, with a spectral resolution <span>({mathcal{R}} approx 250{,}000)</span> and signal-to-noise ratio of about 733:1. The temporal evolution of the Fraunhofer Na <span>i</span> D doublet at <span>(lambda )</span>5890/5896 Å is analyzed using contrast profiles that illustrate subtle changes in the spectral line, not obvious in the intensity profiles. Line bisectors are used to study the height-dependent signature of convective motions. Sun-as-a-star spectra illustrate the radial atmospheric stratification and are affected by limb darkening, solar differential rotation, convective motions, and magnetic activity. During a partial solar eclipse, the contribution of these features is modified by the passage of the Moon, resulting in a transit spectral signature. These observations are compared with synthetic Na <span>i</span> D spectra generated by the Spectropolarimetic NLTE Analytically Powered Inversion (SNAPI) code, based on state-of-the-art Bifrost atmospheric parameters, applied to a geometrically accurate model of the solar eclipse. The model is in qualitative agreement with the observations. However, the discrepancies indicate that models need to be improved, where high-resolution eclipse spectroscopy can serve as a benchmark.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142219148","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-09-02DOI: 10.1007/s11207-024-02366-z
Jirui Yu, Yinghong He, Jinyou Tao, Yang Su, Zhe Zhang, Jianfeng Yang, Nange Wang, Song Guo, Baogang Lv, Xiaobo Chen, Bin Xue, Yiming Hu, Dengyi Chen, Fu Yu, Mingde Ding, Ping Ruan
The ASO-S/HXI is a bi-grids modulating instrument for solar hard X-ray imaging, whose collimator contains 91 pairs of tungsten grids. Since the solar disk is invisible in hard X-rays, a Solar Aspect System (SAS) is required to provide the pointing of hard X-ray imager (HXI) for locating X-ray sources on the solar disk. In addition, the knowledge of the alignment and relative twist of the corresponding front–rear grid pairs is important for image reconstruction as well as locating flares. Therefore, the SAS system was designed to monitor the alignment status of HXI grids and to provide the pointing direction of the HXI collimator with two subsystems DM and SA during the whole life cycle of HXI. DM measures the centroids of the front frosted glasses and the solar disk. SA images the Sun and provides precise relative locations of the solar disk center. Both work in the visible light of 565–585 nm. With all the data together, we can solve with an inversion algorithm the alignment status of the front and rear grids, the relative twist, and the pointing direction. We tested and validated the SAS design with both the simulation model and ground coordinate measuring machine. Here we present the detailed system design, the testing results, the inversion algorithm, and the in-orbit status of the SAS. Currently, the SAS has realized the rotational measurement accuracy of about 4 arcsec, and a translational measurement accuracy of about 15 μm, and the SAS pointing data has been used in both imaging calibration for flare locations and imaging corrections for the platform drifting effect. The high-cadence precise measurement (better than 0.3 arcsec) of the pointing will allow the study of source locations at different energies and therefore help us to understand electron acceleration and transportation in flares.
ASO-S/HXI 是用于太阳硬 X 射线成像的双栅调制仪器,其准直器包含 91 对钨栅。由于太阳圆盘在硬 X 射线中是不可见的,因此需要一个太阳视角系统(SAS)来提供硬 X 射线成像仪(HXI)的指向,以确定太阳圆盘上 X 射线源的位置。此外,了解相应前后网格对的排列和相对扭转对图像重建和耀斑定位也很重要。因此,设计了 SAS 系统来监测 HXI 栅格的对准状态,并通过 DM 和 SA 两个子系统在 HXI 的整个生命周期内提供 HXI 准直器的指向方向。DM 测量前磨砂玻璃和太阳圆盘的中心点。SA 对太阳进行成像,并提供太阳盘中心的精确相对位置。两者都在 565-585 纳米的可见光范围内工作。有了所有的数据,我们就可以用反演算法来解决前后网格的对准状态、相对扭转和指向方向问题。我们利用仿真模型和地面坐标测量机对 SAS 设计进行了测试和验证。在此,我们将介绍详细的系统设计、测试结果、反演算法以及 SAS 的在轨状态。目前,SAS 已经实现了约 4 弧秒的旋转测量精度和约 15 μm 的平移测量精度,SAS 指向数据已用于耀斑位置的成像校准和平台漂移效应的成像修正。高密度精确测量(优于 0.3 弧秒)的指向将允许研究不同能量下的源位置,从而帮助我们了解耀斑中的电子加速和传输。
{"title":"The Solar Aspect System of the Hard X-ray Imager Onboard ASO-S","authors":"Jirui Yu, Yinghong He, Jinyou Tao, Yang Su, Zhe Zhang, Jianfeng Yang, Nange Wang, Song Guo, Baogang Lv, Xiaobo Chen, Bin Xue, Yiming Hu, Dengyi Chen, Fu Yu, Mingde Ding, Ping Ruan","doi":"10.1007/s11207-024-02366-z","DOIUrl":"10.1007/s11207-024-02366-z","url":null,"abstract":"<div><p>The ASO-S/HXI is a bi-grids modulating instrument for solar hard X-ray imaging, whose collimator contains 91 pairs of tungsten grids. Since the solar disk is invisible in hard X-rays, a Solar Aspect System (SAS) is required to provide the pointing of hard X-ray imager (HXI) for locating X-ray sources on the solar disk. In addition, the knowledge of the alignment and relative twist of the corresponding front–rear grid pairs is important for image reconstruction as well as locating flares. Therefore, the SAS system was designed to monitor the alignment status of HXI grids and to provide the pointing direction of the HXI collimator with two subsystems DM and SA during the whole life cycle of HXI. DM measures the centroids of the front frosted glasses and the solar disk. SA images the Sun and provides precise relative locations of the solar disk center. Both work in the visible light of 565–585 nm. With all the data together, we can solve with an inversion algorithm the alignment status of the front and rear grids, the relative twist, and the pointing direction. We tested and validated the SAS design with both the simulation model and ground coordinate measuring machine. Here we present the detailed system design, the testing results, the inversion algorithm, and the in-orbit status of the SAS. Currently, the SAS has realized the rotational measurement accuracy of about 4 arcsec, and a translational measurement accuracy of about 15 μm, and the SAS pointing data has been used in both imaging calibration for flare locations and imaging corrections for the platform drifting effect. The high-cadence precise measurement (better than 0.3 arcsec) of the pointing will allow the study of source locations at different energies and therefore help us to understand electron acceleration and transportation in flares.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s11207-024-02366-z.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142219048","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-30DOI: 10.1007/s11207-024-02362-3
Long Gong, Yunfei Yang, Song Feng, Wei Dai, Bo Liang, Jianping Xiong
Solar active regions serve as the primary energy sources of various solar activities, directly impacting the terrestrial environment. Therefore precise detection and tracking of active regions are crucial for space weather monitoring and forecasting. In this study, a total of 4577 HMI and MDI longitudinal magnetograms are selected for building the dataset, including the training set, validating set, and ten testing sets. They represent different observation instruments, different numbers of activity regions, and different time intervals. A new deep learning method, ReDetGraphTracker, is proposed for detecting and tracking the active regions in full-disk magnetograms. The cooperative modules, especially the redetection module, NSA Kalman filter, and the splitter module, better solve the problems of missing detection, discontinuous trajectory, drifting tracking bounding box, and ID change. The evaluation metrics IDF1, MOTA, MOTP, IDs, and FPS for the testing sets with 24-h interval on average are 74.0%, 74.7%, 0.130, 13.6, and 13.6, respectively. With the decreasing intervals, the metrics become better and better. The experimental results show that ReDetGraphTracker has a good performance in detecting and tracking active regions, especially capturing an active region as early as possible and terminating tracking in near-real time. It can well deal with the active regions whatever evolve drastically or with weak magnetic field strengths, in a near-real-time mode.
{"title":"Solar Active Regions Detection and Tracking Based on Deep Learning","authors":"Long Gong, Yunfei Yang, Song Feng, Wei Dai, Bo Liang, Jianping Xiong","doi":"10.1007/s11207-024-02362-3","DOIUrl":"10.1007/s11207-024-02362-3","url":null,"abstract":"<div><p>Solar active regions serve as the primary energy sources of various solar activities, directly impacting the terrestrial environment. Therefore precise detection and tracking of active regions are crucial for space weather monitoring and forecasting. In this study, a total of 4577 HMI and MDI longitudinal magnetograms are selected for building the dataset, including the training set, validating set, and ten testing sets. They represent different observation instruments, different numbers of activity regions, and different time intervals. A new deep learning method, ReDetGraphTracker, is proposed for detecting and tracking the active regions in full-disk magnetograms. The cooperative modules, especially the redetection module, NSA Kalman filter, and the splitter module, better solve the problems of missing detection, discontinuous trajectory, drifting tracking bounding box, and ID change. The evaluation metrics <i>IDF1</i>, <i>MOTA</i>, <i>MOTP</i>, <i>IDs,</i> and <i>FPS</i> for the testing sets with 24-h interval on average are 74.0%, 74.7%, 0.130, 13.6, and 13.6, respectively. With the decreasing intervals, the metrics become better and better. The experimental results show that ReDetGraphTracker has a good performance in detecting and tracking active regions, especially capturing an active region as early as possible and terminating tracking in near-real time. It can well deal with the active regions whatever evolve drastically or with weak magnetic field strengths, in a near-real-time mode.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 8","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142219149","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2024-08-30DOI: 10.1007/s11207-024-02367-y
Vicki L. Herde, Phillip C. Chamberlin, Don Schmit, Adrian Daw, Ryan O. Milligan, Vanessa Polito, Souvik Bose, Spencer Boyajian, Paris Buedel, Will Edgar, Alex Gebben, Qian Gong, Ross Jacobsen, Nicholas Nell, Bennet Schwab, Alan Sims, David Summers, Zachary Turner, Trace Valade, Joseph Wallace
The Solar eruptioN Integral Field Spectrograph (SNIFS) is a solar-gazing spectrograph scheduled to fly in the summer of 2025 on a NASA sounding rocket. Its goal is to view the solar chromosphere and transition region at a high cadence (1 s) both spatially ((0.5'')) and spectrally (33 mÅ) viewing wavelengths around Lyman alpha (1216 Å), Si iii (1206 Å), and O v (1218 Å) to observe spicules, nanoflares, and possibly a solar flare. This time cadence will provide yet-unobserved detail about fast-changing features of the Sun. The instrument is comprised of a Gregorian-style reflecting telescope combined with a spectrograph via a specialized mirrorlet array that focuses the light from each spatial location in the image so that it may be spectrally dispersed without overlap from neighboring locations. This paper discusses the driving science, detailed instrument and subsystem design, and preintegration testing of the SNIFS instrument.
{"title":"The Solar EruptioN Integral Field Spectrograph","authors":"Vicki L. Herde, Phillip C. Chamberlin, Don Schmit, Adrian Daw, Ryan O. Milligan, Vanessa Polito, Souvik Bose, Spencer Boyajian, Paris Buedel, Will Edgar, Alex Gebben, Qian Gong, Ross Jacobsen, Nicholas Nell, Bennet Schwab, Alan Sims, David Summers, Zachary Turner, Trace Valade, Joseph Wallace","doi":"10.1007/s11207-024-02367-y","DOIUrl":"10.1007/s11207-024-02367-y","url":null,"abstract":"<div><p>The Solar eruptioN Integral Field Spectrograph (SNIFS) is a solar-gazing spectrograph scheduled to fly in the summer of 2025 on a NASA sounding rocket. Its goal is to view the solar chromosphere and transition region at a high cadence (1 s) both spatially (<span>(0.5'')</span>) and spectrally (33 mÅ) viewing wavelengths around Lyman alpha (1216 Å), Si <span>iii</span> (1206 Å), and O <span>v</span> (1218 Å) to observe spicules, nanoflares, and possibly a solar flare. This time cadence will provide yet-unobserved detail about fast-changing features of the Sun. The instrument is comprised of a Gregorian-style reflecting telescope combined with a spectrograph via a specialized mirrorlet array that focuses the light from each spatial location in the image so that it may be spectrally dispersed without overlap from neighboring locations. This paper discusses the driving science, detailed instrument and subsystem design, and preintegration testing of the SNIFS instrument.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 8","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-08-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC11364598/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142103269","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}