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2,423 result(s) for "Solar protons"
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Short-term solar eruptive activity prediction models based on machine learning approaches: A review
Solar eruptive activities, mainly including solar flares, coronal mass ejections (CME), and solar proton events (SPE), have an important impact on space weather and our technosphere. The short-term solar eruptive activity prediction is an active field of research in the space weather prediction. Numerical, statistical, and machine learning methods are proposed to build prediction models of the solar eruptive activities. With the development of space-based and ground-based facilities, a large amount of observational data of the Sun is accumulated, and data-driven prediction models of solar eruptive activities have made a significant progress. In this review, we briefly introduce the machine learning algorithms applied in solar eruptive activity prediction, summarize the prediction modeling process, overview the progress made in the field of solar eruptive activity prediction model, and look forward to the possible directions in the future.
Multiradionuclide evidence for an extreme solar proton event around 2,610 B.P. (∼660 BC)
Recently, it has been confirmed that extreme solar proton events can lead to significantly increased atmospheric production rates of cosmogenic radionuclides. Evidence of such events is recorded in annually resolved natural archives, such as tree rings [carbon-14 (14C)] and ice cores [beryllium-10 (10Be), chlorine-36 (36Cl)]. Here, we show evidence for an extreme solar event around 2,610 years B.P. (∼660 BC) based on high-resolution 10Be data from two Greenland ice cores. Our conclusions are supported by modeled 14C production rates for the same period. Using existing 36Cl ice core data in conjunction with 10Be, we further show that this solar event was characterized by a very hard energy spectrum. These results indicate that the 2,610-years B.P. event was an order of magnitude stronger than any solar event recorded during the instrumental period and comparable with the solar proton event of AD 774/775, the largest solar event known to date. The results illustrate the importance of multiple ice core radionuclide measurements for the reliable identification of short-term production rate increases and the assessment of their origins.
Characterizing High-Energy Solar Proton Events with Energies Below and Above 100 MeV
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 ∼ 68  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. The coronal mass ejections (CMEs) associated with > 100  MeV proton events appeared to be, on average, more energetic than those associated with < 100  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 > 100  MeV proton events, protons were released over the rise phase of the SXR flares, whereas in most of the < 100  MeV events the proton releases occurred after the peak of the SXR flares. We established limits for the CME speed V CME and SXR peak flux F pk or total fluence F i , which helped us to distinguish the events in the two groups. Solar eruptions with V CME > 1000  km s −1 and F > pk 5 ⋅ 10 − 5  W m −2 had a high probability to produce proton events of > 100  MeV. On the other hand, eruptions with V > CME 900  km s −1 and F < i 5 ⋅ 10 − 4  J m −2 and eruptions with V < CME 900  km s −1 irrespective of the SXR total fluence were very likely to produce proton events of < 100  MeV. 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 < 100  MeV proton events while they were observed in 88% of > 100  MeV events. Our analysis showed that protons in most of the > 100  MeV events were released low in the corona ( ≤ 3.0 R ⊙ ) before the onsets of the DH-Type II radio bursts. Conversely, protons in most of the < 100  MeV events were released higher in the corona ( > 3 R ⊙ ) and after the DH-Type II onsets. We conclude that protons in most of the > 100  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 < 100  MeV events, protons are mainly accelerated in CME shocks at coronal heights > 3 R ⊙ .
Comparing Data on the Times of Solar Proton Release in Solar Proton Events, Obtained in Different Ways
Times of the release of solar unrelativistic protons, determined from the scale invariance of temporal profiles of solar proton events, are compared to results from studies in which the times of release for solar relativistic protons in GLE events are determined through velocity dispersion and the initial observation on neutron monitors, allowing for the dependence of the length of Sun‒Earth magnetic lines on the velocity of the solar wind.
Extremely active Sun from 1190 to 1220 in the Medieval Period: Intercomparison of historical records and tree-ring carbon-14
Several large sunspots and red aurorae have been recorded in the literature from relatively low geomagnetic latitude regions in Northeast Asia around 1200–1205 CE, and this interval can be regarded as one of the highest solar activity periods in the Medieval Period. To search for a potential solar proton event during this time and examine the solar cycle dependence, a high-precision carbon-14 analysis with annual resolution was conducted. We found no enhancement in carbon-14 around 1204 CE when prolonged low-latitude aurorae were observed in Kyoto, Japan, as recorded in Meigetsuki. Instead, we found a potential solar proton event in 1200–1201 CE, possibly associated with either the large sunspots or the red auroral events documented in this period. Reconstruction of solar cycles around the event suggested that this solar proton event occurred at the activity cycle’s maximum. We also found that the solar cycles around this period were approximately seven to eight years, much shorter than those in the modern era, suggesting extremely high solar activity.
Variations in Characteristics of the Northern Hemisphere’s Middle Atmosphere during Solar Proton Events of January 2005
Data from the MERRA-2 archive were used to study characteristics of the Northern Hemisphere’s middle atmosphere during the solar proton events of January 2005. It was found that the events were accompanied by sharp changes in zonal wind speed and temperature in the high-latitude atmosphere. The results obtained provide evidence of an intensification of the stratospheric polar vortex during the events, which was followed by a sharp weakening of the vortex and the development of a stratospheric warming.
Magnetosphere-Ground Responses and Energy Spectra Analysis of Solar Proton Event on 28 October 2021
Among the coronal mass ejections (CMEs) and solar proton events (SPEs) frequently observed by near-Earth spacecraft, the SPE that occurred on 28 October 2021 stands out as a remarkable research event. This is due to the infrequency of reported ground-level enhancements it induced. The CSES (China seismo-electromagnetic satellite) is equipped with high-energy particle detectors, namely, HEPP and HEPD, capable of measuring protons within an energy range of 2 MeV to 143 MeV. These detectors provide valuable opportunities for studying solar activity. By utilizing the Monte Carlo method to simulate the pile-up effect and accounting for the detector’s dead time, with the assistance of real-time incident counting rates, we successfully corrected the spectra in the 10–50 MeV range. The energy spectrum is important for understanding solar proton events. We used the data from the HEPP (high-energy particle package) and HEPD (high-energy particle detector) to obtain the total event-integrated spectrum, which possessed good continuity. Additionally, we compared the observations from the CSES with those from the NOAA satellite and achieved reasonable agreement. We also searched for ground-based responses to this solar activity in China and discovered Forbush decreases detected by the Yang Ba Jing Muon Telescope experiment. In conclusion, the HEPP and HEPD can effectively combine to study solar activity and obtain a smooth and consistent energy spectrum of protons across a very wide energy range.
RADIOCARBON VARIATIONS IN ANNUAL TREE RINGS WITH 11-YEAR SOLAR CYCLES DURING 1800–1950
The results of radiocarbon variation studies observed in annual tree rings from the NW Pacific (USA Northwest) (Stuiver and Braziunas 1993) and Europe (England, Brehm et al. 2021; Slovakia, Povinec 1977, 1987) are reviewed with the aim of better understanding the 11-year radiocarbon cycle and possible impacts of solar proton events on 14C levels in the atmosphere and biosphere. The average Δ14C amplitude in tree rings for the period of 1798–1944 was 1.3 ± 0.3‰, the average periodicity was 11 ± 1 years, and the average time shift between the sunspot numbers and Δ14C records was 3 ± 1 years. A new solar activity minimum (Gleissberg minimum, 1878–1933) has been identified in the Δ14C data sets from the NW Pacific and England, showing Δ14C excess of 7‰, comparable to the Dalton minimum (1797–1823). No significant changes in Δ14C levels were identified that could be associated with solar proton events during 1800–1950.
Geomagnetic Storm Effects on the LEO Proton Flux During Solar Energetic Particle Events
During a few solar energetic particle (SEP) events, solar protons were trapped within the geomagnetic field and reached the outer edge of the inner radiation belt. We reproduced this phenomenon by modeling the proton flux distribution at the Low‐Earth Orbit (LEO) for different geomagnetic conditions during solar particle events. We developed a three‐dimensional relativistic test particle simulation code to compute the 70–180 MeV solar proton Lorentz trajectories in low L‐shell range from 1 to 3. The Tsyganenko model (T01) generated the background static magnetic field with the IGRF (v12) model. We have selected three Dst index values: −7, −150, and −210 nT, to define quiet time, strong, and severe geomagnetic storms and to generate the corresponding inner magnetic field configurations. Our results showed that the simulated solar proton flux was more enhanced in the high‐latitude regions and more expanded toward the lower latitude range as long as the geomagnetic storm was intensified. Satellite observations and geomagnetic cutoff rigidities confirmed the numerical results. Furthermore, the LEO proton flux distribution was deformed, so the structure of the proton flux inside the South Atlantic Anomaly (SAA) became longitudinally extended as the Dst index decreased. Moreover, we have assessed the corresponding radiation environment of the LEO mission. We realized that, for a higher inclined LEO mission during an intense geomagnetic storm (Dst = −210 nT), the probability of the occurrence of the Single Event Upset (SEU) rates increased by 19% and the estimated accumulated absorbed radiation doses increased by 17% in comparison with quiet conditions.
Influence of Processes on the Sun and in the Interplanetary Medium on the Solar Proton Event on March 30, 2022
The article presents the results of a comparative analysis of the solar proton event on March 30, 2022, which has an unusual time profile of solar proton fluxes, and the previous and subsequent solar proton events (March 28, 2022, and April 02, 2022). Increases in energetic proton fluxes in the interplanetary and near-Earth space are associated with successive solar X-ray flares M4.0, X1.3, and M3.9 and three halo-type coronal mass ejections. The study was based on experimental data obtained from spacecraft located in the interplanetary space (ACE, WIND, STEREO A, and DSCOVR), in a circular polar orbit at an altitude of 850 km (Meteor-M2) and in geostationary orbit (GOES-16, Electro-L2). An explanation has been proposed for the specific features of the energetic proton flux profile in the solar proton event on March 30, 2022: protons accelerated in the flare on March 30, 2022 were partially screened by an interplanetary coronal mass ejection, the source of which was the explosive processes on the Sun on March 28, 2022; late detection of maximum proton fluxes, simultaneous for particles of different energies, is due to the arrival of particle fluxes inside an interplanetary coronal mass ejection. The spatial distribution of solar protons in near-Earth orbit was similar to the distribution at the Lagrange point L1 but with a delay of ~50 min.