The problem of coronal heating is one of the fundamental problems of solar physics. At present, it is again attracting great interest due to the appearance of a large amount of observational data of high spatial and temporal resolution. These data made it possible to diagnose plasma parameters from observations of waves and oscillations in coronal magnetic structures and, moreover, to introduce analytical constraints on the coronal heating function. In this paper, we propose an approach allowing us to impose constraints on the heating function based on data on the gravitational stratification of the solar atmosphere. The developed algorithm is applied to the altitude profiles of temperature and density in several regions of the solar corona obtained from direct modeling of EUV radiation from the Solar Dynamics Observatory/Atmospheric Imaging Assembly (SDO/AIA). Assuming that the heating function is a power function of temperature and density, we determine the domain of power-index constraints allowing us to realize the observed altitude profiles. The obtained results are combined with the conditions of stability for the entropy and magnetoacoustic modes, to narrow the region of possible parameters further.
{"title":"Diagnostics of Solar Corona Heating Parameters Using the Observed Gravitational Stratification of the Medium","authors":"Dmitrii Riashchikov, Elizaveta Scoptsova, Dmitrii Zavershinskii","doi":"10.1007/s11207-024-02383-y","DOIUrl":"10.1007/s11207-024-02383-y","url":null,"abstract":"<div><p>The problem of coronal heating is one of the fundamental problems of solar physics. At present, it is again attracting great interest due to the appearance of a large amount of observational data of high spatial and temporal resolution. These data made it possible to diagnose plasma parameters from observations of waves and oscillations in coronal magnetic structures and, moreover, to introduce analytical constraints on the coronal heating function. In this paper, we propose an approach allowing us to impose constraints on the heating function based on data on the gravitational stratification of the solar atmosphere. The developed algorithm is applied to the altitude profiles of temperature and density in several regions of the solar corona obtained from direct modeling of EUV radiation from the <i>Solar Dynamics Observatory/Atmospheric Imaging Assembly</i> (SDO/AIA). Assuming that the heating function is a power function of temperature and density, we determine the domain of power-index constraints allowing us to realize the observed altitude profiles. The obtained results are combined with the conditions of stability for the entropy and magnetoacoustic modes, to narrow the region of possible parameters further.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-27","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142414436","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 : 2024-09-25DOI: 10.1007/s11207-024-02379-8
Tom Narock, Sanchita Pal, Aryana Arsham, Ayris Narock, Teresa Nieves-Chinchilla
Decades of in-situ solar-wind measurements have clearly established the variation of solar-wind physical parameters. These variable parameters have been used to classify the solar-wind magnetized plasma into different types, leading to several classification schemes being developed. These classification schemes, while useful for understanding the solar wind’s originating processes at the Sun and early detection of space weather events, have left open questions regarding which physical parameters are most useful for classification and how recent advances in our understanding of solar-wind transients impact classification. In this work, we use neural networks trained with different solar-wind magnetic and plasma characteristics to automatically classify the solar wind in coronal hole, streamer belt, sector reversal and solar transients such as coronal mass ejections comprised of both magnetic obstacles and sheaths. Furthermore, our work demonstrates how probabilistic neural networks can enhance the classification by including a measure of prediction uncertainty. Our work also provides a ranking of the parameters that lead to an improved classification scheme with (sim 96%) accuracy. Our new scheme paves the way for incorporating uncertainty estimates into space-weather forecasting with the potential to be implemented on real-time solar-wind data.
{"title":"Classifying Different Types of Solar-Wind Plasma with Uncertainty Estimations Using Machine Learning","authors":"Tom Narock, Sanchita Pal, Aryana Arsham, Ayris Narock, Teresa Nieves-Chinchilla","doi":"10.1007/s11207-024-02379-8","DOIUrl":"10.1007/s11207-024-02379-8","url":null,"abstract":"<div><p>Decades of in-situ solar-wind measurements have clearly established the variation of solar-wind physical parameters. These variable parameters have been used to classify the solar-wind magnetized plasma into different types, leading to several classification schemes being developed. These classification schemes, while useful for understanding the solar wind’s originating processes at the Sun and early detection of space weather events, have left open questions regarding which physical parameters are most useful for classification and how recent advances in our understanding of solar-wind transients impact classification. In this work, we use neural networks trained with different solar-wind magnetic and plasma characteristics to automatically classify the solar wind in coronal hole, streamer belt, sector reversal and solar transients such as coronal mass ejections comprised of both magnetic obstacles and sheaths. Furthermore, our work demonstrates how probabilistic neural networks can enhance the classification by including a measure of prediction uncertainty. Our work also provides a ranking of the parameters that lead to an improved classification scheme with <span>(sim 96%)</span> accuracy. Our new scheme paves the way for incorporating uncertainty estimates into space-weather forecasting with the potential to be implemented on real-time solar-wind data.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142413668","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 : 2024-09-25DOI: 10.1007/s11207-024-02378-9
Dheyaa Ameri, Eino Valtonen, Amjad Al-Sawad, Rami Vainio
<div><p>We analyzed 58 high-energy proton events that occurred during the years 1996 – 2022. In 32 out of the 58 (55%) events, the proton energies extended up to <span>(sim 68)</span> MeV but did not reach 100 MeV. In the remaining 26 events, the proton energies exceeded 100 MeV. We studied the differences in the characteristics of these proton events and their associations with solar and interplanetary phenomena to improve understanding proton sources and acceleration processes.</p><p>The coronal mass ejections (CMEs) associated with <span>(>100)</span> MeV proton events appeared to be, on average, more energetic than those associated with <span>(< 100)</span> MeV proton events. The peak and integrated fluxes (fluence) of the soft X-ray (SXR) flares were higher in > 100 MeV proton events, but there was almost no difference in the rise times of the flares. In a major part of the <span>(> 100)</span> MeV proton events, protons were released over the rise phase of the SXR flares, whereas in most of the <span>(<100)</span> MeV events the proton releases occurred after the peak of the SXR flares. We established limits for the CME speed V<sub>CME</sub> and SXR peak flux F<sub>pk</sub> or total fluence F<sub><i>i</i></sub>, which helped us to distinguish the events in the two groups. Solar eruptions with V<sub>CME</sub> <span>(> 1000)</span> km s<sup>−1</sup> and F<span>(_{mathrm{pk}} > 5 cdot 10^{-5} )</span> W m<sup>−2</sup> had a high probability to produce proton events of <span>(> 100)</span> MeV. On the other hand, eruptions with V<span>(_{mathrm{CME}} > 900)</span> km s<sup>−1</sup> and F<span>(_{i} <5 cdot 10^{-4} )</span> J m<sup>−2</sup> and eruptions with V<span>(_{ mathrm{CME}} < 900)</span> km s<sup>−1</sup> irrespective of the SXR total fluence were very likely to produce proton events of <span>(< 100)</span> MeV.</p><p>All proton events were associated with decametric Type III radio bursts, and most of them had Type II bursts associations either in metric or decametric–hectometric (DH) wavelengths or both. Both metric- and DH-Type II emissions were observed in 50% of <span>(<100)</span> MeV proton events while they were observed in 88% of <span>(>100)</span> MeV events. Our analysis showed that protons in most of the <span>(>100)</span> MeV events were released low in the corona (<span>(leq 3.0)</span> R<sub>⊙</sub>) before the onsets of the DH-Type II radio bursts. Conversely, protons in most of the <span>(<100)</span> MeV events were released higher in the corona (<span>(>3)</span> R<sub>⊙</sub>) and after the DH-Type II onsets.</p><p>We conclude that protons in most of the <span>(> 100)</span> MeV events are accelerated either by the flare reconnection processes or by shocks low in the corona and could undergo reacceleration higher in the corona in CME shocks manifested in DH-Type II radio emission. In the <span>(<100)</span> MeV events, protons are mainly accelerated in CME sho
{"title":"Characterizing High-Energy Solar Proton Events with Energies Below and Above 100 MeV","authors":"Dheyaa Ameri, Eino Valtonen, Amjad Al-Sawad, Rami Vainio","doi":"10.1007/s11207-024-02378-9","DOIUrl":"10.1007/s11207-024-02378-9","url":null,"abstract":"<div><p>We analyzed 58 high-energy proton events that occurred during the years 1996 – 2022. In 32 out of the 58 (55%) events, the proton energies extended up to <span>(sim 68)</span> MeV but did not reach 100 MeV. In the remaining 26 events, the proton energies exceeded 100 MeV. We studied the differences in the characteristics of these proton events and their associations with solar and interplanetary phenomena to improve understanding proton sources and acceleration processes.</p><p>The coronal mass ejections (CMEs) associated with <span>(>100)</span> MeV proton events appeared to be, on average, more energetic than those associated with <span>(< 100)</span> MeV proton events. The peak and integrated fluxes (fluence) of the soft X-ray (SXR) flares were higher in > 100 MeV proton events, but there was almost no difference in the rise times of the flares. In a major part of the <span>(> 100)</span> MeV proton events, protons were released over the rise phase of the SXR flares, whereas in most of the <span>(<100)</span> MeV events the proton releases occurred after the peak of the SXR flares. We established limits for the CME speed V<sub>CME</sub> and SXR peak flux F<sub>pk</sub> or total fluence F<sub><i>i</i></sub>, which helped us to distinguish the events in the two groups. Solar eruptions with V<sub>CME</sub> <span>(> 1000)</span> km s<sup>−1</sup> and F<span>(_{mathrm{pk}} > 5 cdot 10^{-5} )</span> W m<sup>−2</sup> had a high probability to produce proton events of <span>(> 100)</span> MeV. On the other hand, eruptions with V<span>(_{mathrm{CME}} > 900)</span> km s<sup>−1</sup> and F<span>(_{i} <5 cdot 10^{-4} )</span> J m<sup>−2</sup> and eruptions with V<span>(_{ mathrm{CME}} < 900)</span> km s<sup>−1</sup> irrespective of the SXR total fluence were very likely to produce proton events of <span>(< 100)</span> MeV.</p><p>All proton events were associated with decametric Type III radio bursts, and most of them had Type II bursts associations either in metric or decametric–hectometric (DH) wavelengths or both. Both metric- and DH-Type II emissions were observed in 50% of <span>(<100)</span> MeV proton events while they were observed in 88% of <span>(>100)</span> MeV events. Our analysis showed that protons in most of the <span>(>100)</span> MeV events were released low in the corona (<span>(leq 3.0)</span> R<sub>⊙</sub>) before the onsets of the DH-Type II radio bursts. Conversely, protons in most of the <span>(<100)</span> MeV events were released higher in the corona (<span>(>3)</span> R<sub>⊙</sub>) and after the DH-Type II onsets.</p><p>We conclude that protons in most of the <span>(> 100)</span> MeV events are accelerated either by the flare reconnection processes or by shocks low in the corona and could undergo reacceleration higher in the corona in CME shocks manifested in DH-Type II radio emission. In the <span>(<100)</span> MeV events, protons are mainly accelerated in CME sho","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s11207-024-02378-9.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142413778","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 : 2024-09-25DOI: 10.1007/s11207-024-02369-w
Laura Jade Millson, Anne-Marie Broomhall, Tishtrya Mehta
At high frequencies beyond the acoustic cut-off, a peak-like structure is visible in the solar power spectrum. Known as the pseudo-modes, their frequencies have been shown to vary in anti-phase with solar magnetic activity. In this work, we determined temporal variations in these frequencies across the solar disc, with the aim of identifying any potential latitudinal dependence of pseudo-mode frequency shifts. We utilised nearly 22 years of spatially resolved GONG data for all azimuthal orders, (textit{m}), for harmonic degrees (0leq lleq 200), and determined shifts using the resampled periodogram method. Periodogram realisations were created from overlapping, successive 216 day-long segments in time, and cropped to 5600 – 6800 μHz. Cross-correlation functions were then repeatedly generated between these realisations to identify any variation in frequency and the uncertainty. We categorised each mode by its latitudinal sensitivity and used this categorisation to produce average frequency shifts for different latitude bands (15∘ and 5∘ in size) which were compared to magnetic proxies, the (F_{mathrm{10.7}}) index and GONG synoptic maps. Morphological differences in the pseudo-mode shifts between different latitudes were found, which were most pronounced during the rise to solar maximum where shifts reach their minimum values. At all latitudes, shift behaviour was strongly in anti-correlation with the activity proxy. Additionally, periodicities shorter than the 11-year cycle were observed. Wavelet analysis was used to identify a periodicity of four years at all latitudes.
{"title":"Latitudinal Dependence of Variations in the Frequencies of Solar Oscillations Above the Acoustic Cut-Off","authors":"Laura Jade Millson, Anne-Marie Broomhall, Tishtrya Mehta","doi":"10.1007/s11207-024-02369-w","DOIUrl":"10.1007/s11207-024-02369-w","url":null,"abstract":"<div><p>At high frequencies beyond the acoustic cut-off, a peak-like structure is visible in the solar power spectrum. Known as the pseudo-modes, their frequencies have been shown to vary in anti-phase with solar magnetic activity. In this work, we determined temporal variations in these frequencies across the solar disc, with the aim of identifying any potential latitudinal dependence of pseudo-mode frequency shifts. We utilised nearly 22 years of spatially resolved GONG data for all azimuthal orders, <span>(textit{m})</span>, for harmonic degrees <span>(0leq lleq 200)</span>, and determined shifts using the resampled periodogram method. Periodogram realisations were created from overlapping, successive 216 day-long segments in time, and cropped to 5600 – 6800 μHz. Cross-correlation functions were then repeatedly generated between these realisations to identify any variation in frequency and the uncertainty. We categorised each mode by its latitudinal sensitivity and used this categorisation to produce average frequency shifts for different latitude bands (15<sup>∘</sup> and 5<sup>∘</sup> in size) which were compared to magnetic proxies, the <span>(F_{mathrm{10.7}})</span> index and GONG synoptic maps. Morphological differences in the pseudo-mode shifts between different latitudes were found, which were most pronounced during the rise to solar maximum where shifts reach their minimum values. At all latitudes, shift behaviour was strongly in anti-correlation with the activity proxy. Additionally, periodicities shorter than the 11-year cycle were observed. Wavelet analysis was used to identify a periodicity of four years at all latitudes.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s11207-024-02369-w.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142413711","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 : 2024-09-25DOI: 10.1007/s11207-024-02380-1
Alexander Kutsenko, Valery Terebizh, Andrei Dolgopolov, Valentina Abramenko, Andrei Plotnikov, Dmitriy Semyonov, Vladimir Skiruta, Vyacheslav Lopukhin
The Spectro-Polarimeter (SP) is a new instrument installed at the upgraded Andrei B. Severny Solar Tower Telescope (STT) at the Crimean Astrophysical Observatory. The instrument is a traditional echelle slit dual-beam spectropolarimeter with temporal modulation of the polarization. STT-SP provides simultaneous spectropolarimetric observations of the Sun within three 15 Å wide spectral ranges around photospheric Fe I 5250 Å, Fe I 5324 Å, and chromospheric Mg I b2 5172 Å spectral lines. The spectral resolution of the instrument reaches 70,000 with the seeing-constrained slit width of 1 arcsec. The field-of-view of STT-SP is 200 arcsec allowing one to map a moderate size active region within a single raster scan. The instrument will provide new opportunities in the analysis of magnetic fields and thermodynamics of the lower atmosphere of the Sun. In this paper we describe the optical design of STT-SP and present the preliminary results acquired during the commissioning of the instrument.
分光偏振计(SP)是安装在克里米亚天体物理观测台升级版 Andrei B. Severny 太阳塔望远镜(STT)上的新仪器。该仪器是一种传统的梯形狭缝双光束分光测偏仪,具有偏振时间调制功能。STT-SP 围绕光球层 Fe I 5250 Å、Fe I 5324 Å 和色球层 Mg I b2 5172 Å 光谱线,在三个 15 Å 宽光谱范围内同时对太阳进行分光测极观测。该仪器的光谱分辨率达到 70,000,视线受限狭缝宽度为 1 弧秒。STT-SP 的视场为 200 弧秒,可以在一次光栅扫描中绘制出中等大小的活动区。该仪器将为分析太阳低层大气的磁场和热力学提供新的机会。在本文中,我们将介绍 STT-SP 的光学设计,并介绍在仪器调试期间获得的初步结果。
{"title":"The Spectro-Polarimeter of the Andrei B. Severny Solar Tower Telescope at the Crimean Astrophysical Observatory: Optical Design and Implementation","authors":"Alexander Kutsenko, Valery Terebizh, Andrei Dolgopolov, Valentina Abramenko, Andrei Plotnikov, Dmitriy Semyonov, Vladimir Skiruta, Vyacheslav Lopukhin","doi":"10.1007/s11207-024-02380-1","DOIUrl":"10.1007/s11207-024-02380-1","url":null,"abstract":"<div><p>The <i>Spectro-Polarimeter</i> (SP) is a new instrument installed at the upgraded <i>Andrei B. Severny Solar Tower Telescope</i> (STT) at the <i>Crimean Astrophysical Observatory</i>. The instrument is a traditional echelle slit dual-beam spectropolarimeter with temporal modulation of the polarization. STT-SP provides simultaneous spectropolarimetric observations of the Sun within three 15 Å wide spectral ranges around photospheric Fe I 5250 Å, Fe I 5324 Å, and chromospheric Mg I b2 5172 Å spectral lines. The spectral resolution of the instrument reaches 70,000 with the seeing-constrained slit width of 1 arcsec. The field-of-view of STT-SP is 200 arcsec allowing one to map a moderate size active region within a single raster scan. The instrument will provide new opportunities in the analysis of magnetic fields and thermodynamics of the lower atmosphere of the Sun. In this paper we describe the optical design of STT-SP and present the preliminary results acquired during the commissioning of the instrument.</p></div>","PeriodicalId":777,"journal":{"name":"Solar Physics","volume":"299 9","pages":""},"PeriodicalIF":2.7,"publicationDate":"2024-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142413773","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}
The torsional Alfvén wave is highly regarded as the carrier of the energy from the photosphere to the corona in the solar atmosphere. This paper presents a comprehensive linear analysis of the wave behavior and energy transfer within an open, twisted, divergent magnetic flux tube configuration, considering the impact of wave guide structure on the propagation of these waves using the magneto-hydrodynamic approach. The study shows that waves with frequencies between 0.001 Hz and 1 Hz can effectively penetrate the transition region, with the most efficient energy transfer occurring in the 0.1 Hz to 1 Hz frequency range. The research findings suggest that waves with certain intermediate frequencies are able to transmit energy to the coronal region of the Sun, contributing to its active heating.
{"title":"A Linear Analysis of Torsional Alfvén Waves in Open Twisted Divergent Magnetic Flux Tubes for Coronal Heating","authors":"Bivek Pradhan, Gobinda Chandra Mishra, Pralay Kumar Karmakar, Utpal Deka","doi":"10.1007/s11207-024-02372-1","DOIUrl":"10.1007/s11207-024-02372-1","url":null,"abstract":"<div><p>The torsional Alfvén wave is highly regarded as the carrier of the energy from the photosphere to the corona in the solar atmosphere. This paper presents a comprehensive linear analysis of the wave behavior and energy transfer within an open, twisted, divergent magnetic flux tube configuration, considering the impact of wave guide structure on the propagation of these waves using the magneto-hydrodynamic approach. The study shows that waves with frequencies between 0.001 Hz and 1 Hz can effectively penetrate the transition region, with the most efficient energy transfer occurring in the 0.1 Hz to 1 Hz frequency range. The research findings suggest that waves with certain intermediate frequencies are able to transmit energy to the coronal region of the Sun, contributing to its active heating.</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/s11207-024-02372-1.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"142412781","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 : 2024-09-20DOI: 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}