Search Publications

A Type II Radio Burst Driven by a Blowout Jet on the Sun
DOI: 10.3847/1538-4357/ace31b Bibcode: 2023ApJ...953..171H

Tian, Hui; Madjarska, Maria S.; Deng, Yuanyong +5 more

Type II radio bursts are often associated with coronal shocks that are typically driven by coronal mass ejections (CMEs) from the Sun. Here we conduct a case study of a type II radio burst that is associated with a C4.5-class flare and a blowout jet, but without the presence of a CME. The blowout jet is observed near the solar disk center in the e…

2023 The Astrophysical Journal
SOHO 17
Deciphering the Slow-rise Precursor of a Major Coronal Mass Ejection
DOI: 10.3847/2041-8213/acf3e4 Bibcode: 2023ApJ...954L..47C

Peter, H.; Solanki, S. K.; Aulanier, G. +3 more

Coronal mass ejections are explosive plasma phenomena prevalently occurring on the Sun and probably on other magnetically active stars. However, how their pre-eruptive configuration evolves toward the main explosion remains elusive. Here, based on comprehensive observations of a long-duration precursor in an event on 2012 March 13, we determine th…

2023 The Astrophysical Journal
SOHO 14
A Database of Magnetic and Thermodynamic Properties of Confined and Eruptive Solar Flares
DOI: 10.3847/1538-4357/ad004e Bibcode: 2023ApJ...958..104K

Kazachenko, Maria D.

Solar flares sometimes lead to coronal mass ejections that directly affect Earth's environment. However, a large fraction of flares, including on solar-type stars, are confined flares. What are the differences in physical properties between confined and eruptive flares? For the first time, we quantify the thermodynamic and magnetic properties of h…

2023 The Astrophysical Journal
SOHO 14
Modeling a Coronal Mass Ejection from an Extended Filament Channel. II. Interplanetary Propagation to 1 au
DOI: 10.3847/1538-4357/ad0229 Bibcode: 2023ApJ...958...91P

Scolini, Camilla; Lynch, Benjamin J.; Palmerio, Erika +5 more

We present observations and modeling results of the propagation and impact at Earth of a high-latitude, extended filament channel eruption that commenced on 2015 July 9. The coronal mass ejection (CME) that resulted from the filament eruption was associated with a moderate disturbance at Earth. This event could be classified as a so-called "proble…

2023 The Astrophysical Journal
SOHO Ulysses 13
Reconstructing the XUV Spectra of Active Sun-like Stars Using Solar Scaling Relations with Magnetic Flux
DOI: 10.3847/1538-4357/acbe38 Bibcode: 2023ApJ...945..147N

Notsu, Yuta; Namekata, Kosuke; Toriumi, Shin +3 more

The Kepler space telescope and Transiting Exoplanet Survey Satellite unveiled that Sun-like stars frequently host exoplanets. These exoplanets are subject to fluxes of ionizing radiation in the form of X-ray and extreme-ultraviolet (EUV) radiation that may cause changes in their atmospheric dynamics and chemistry. While X-ray fluxes can be observe…

2023 The Astrophysical Journal
Gaia IUE SOHO eHST 13
The Eruption of a Magnetic Flux Rope Observed by Solar Orbiter and Parker Solar Probe
DOI: 10.3847/1538-4357/acefd5 Bibcode: 2023ApJ...955..152L

Long, David M.; Davies, Emma E.; Berghmans, David +11 more

Magnetic flux ropes are a key component of coronal mass ejections, forming the core of these eruptive phenomena. However, determining whether a flux rope is present prior to eruption onset and, if so, the rope's handedness and the number of turns that any helical field lines make is difficult without magnetic field modeling or in situ detection of…

2023 The Astrophysical Journal
SOHO SolarOrbiter 12
On the Nature of the Three-part Structure of Solar Coronal Mass Ejections
DOI: 10.3847/1538-4357/aca6e0 Bibcode: 2023ApJ...942...19S

Chen, Yao; Xia, Lidong; Li, Leping +4 more

Coronal mass ejections (CMEs) result from eruptions of magnetic flux ropes (MFRs) and can possess a three-part structure in white-light coronagraphs, including a bright front, dark cavity, and bright core. In traditional opinion, the bright front forms due to the plasma pileup along the MFR border, the cavity represents the cross section of the MF…

2023 The Astrophysical Journal
SOHO 11
What Do Halo CMEs Tell Us about Solar Cycle 25?
DOI: 10.3847/2041-8213/acdde2 Bibcode: 2023ApJ...952L..13G

Gopalswamy, Nat; Akiyama, Sachiko; Yashiro, Seiji +3 more

It is known that the weak state of the heliosphere due to diminished solar activity in cycle 24 backreacted on coronal mass ejections (CMEs) to make them appear wider for a given speed. One of the consequences of the weak state of the heliosphere is that more CMEs appear as halo CMEs (HCMEs), and halos are formed at shorter heliocentric distances.…

2023 The Astrophysical Journal
SOHO 11
Understanding the Lateral Drifting of an Erupting Filament with a Data-constrained Magnetohydrodynamic Simulation
DOI: 10.3847/1538-4357/acf198 Bibcode: 2023ApJ...956..119G

Schmieder, B.; Poedts, S.; Li, C. +6 more

Solar filaments often exhibit rotation and deflection during eruptions, which would significantly affect the geoeffectiveness of the corresponding coronal mass ejections (CMEs). Therefore, understanding the mechanisms that lead to such rotation and lateral displacement of filaments is a great concern to space weather forecasting. In this paper, we…

2023 The Astrophysical Journal
SOHO 11
On the Connection between Rieger-type and Magneto-Rossby Waves Driving the Frequency of the Large Solar Eruptions during Solar Cycles 19-25
DOI: 10.3847/1538-4357/acb64f Bibcode: 2023ApJ...944..180K

Korsós, Marianna B.; Liu, Jiajia; Erdélyi, Robertus +2 more

Global solar activity variation mainly occurs over about an 11 yr cycle. However, both longer and shorter periodicities than the solar cycle are also present in many different solar activity indices. The longer timescales may be up to hundreds of years, while the shorter timescales for global solar variability could be within 0.5-2 yr, which inclu…

2023 The Astrophysical Journal
SOHO 10