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In \citet{Stangalini20} and \citet{Deb20}, magnetic oscillations were detected in the chromosphere of a large sunspot and found to be linked to the coronal locations where a First Ionization Potential (FIP) effect was observed. In an…

We report X-ray spectroscopic results for four giant solar flares occurred on 2005 September 7 (X17.0), 2005 September 8 (X5.4), 2005 September 9 (X6.2), and 2006 December 5 (X9.0), obtained from Earth albedo data with the X-ray imaging…

We present measurements of elemental abundances in solar flares with the EUV Variability Experiment (EVE) on the Solar Dynamics Observatory (SDO). EVE observes both high temperature Fe emission lines (Fe XV-Fe XXIV) and continuum emission…

Solar and Stellar Astrophysics · Physics 2015-06-17 Harry P. Warren

A Chandra spectrum of the moderately active nearby F6 V star Pi3 Ori is used to study the coronal properties of mid-F dwarfs. We find that Pi3 Ori's coronal emission measure distribution is very similar to those of moderately active G and K…

Solar and Stellar Astrophysics · Physics 2015-06-15 Brian E. Wood , J. Martin Laming

The studies on the origination and generation mechanisms of ICME materials are crucial for understanding the connection between CMEs and flares. The materials inside ICMEs can be classified into three types, coming from corona directly…

Solar and Stellar Astrophysics · Physics 2023-09-19 Hui Fu , Xinzheng Shi , Zhenghua Huang , Youqian Qi , Lidong Xia

On 2008 May 2, Chandra observed the X-ray spectrum of Xi Boo (G8 V+K4 V), resolving the binary for the first time in X-rays and allowing the coronae of the two stars to be studied separately. With the contributions of Xi Boo A and B to the…

Solar and Stellar Astrophysics · Physics 2015-05-19 Brian E. Wood , Jeffrey L. Linsky

The calcium abundance in flare plasmas is estimated using X-ray spectra from the Solar Maximum Mission Bent Crystal Spectrometer (BCS) during the decays of 194 flares (GOES classifications from B6.4 to X13) occurring between 1980 and 1989.…

Solar and Stellar Astrophysics · Physics 2022-05-18 J. Sylwester , B. Sylwester , K. J. H. Phillips , A. Kepa

The composition of plasma in the solar corona is characterised by the First Ionisation Potential (FIP) bias, and is thought to be the result of a ponderomotive force acting in the chromosphere to separate ionised from neutral plasma.…

Solar and Stellar Astrophysics · Physics 2026-03-06 Éabha Power , David M. Long , Teodora Mihailescu , Laura A. Hayes

The elemental composition of the solar wind differs from the solar photospheric composition. Elements with low first ionization potential (FIP) appear enhanced compared to O in the solar wind relative to the respective photospheric…

Solar and Stellar Astrophysics · Physics 2018-11-14 Verena Heidrich-Meisner , Lars Berger , Robert F. Wimmer-Schweingruber

The RESIK instrument on {\em CORONAS-F} spacecraft observed several sulphur X-ray lines in three of its four channels covering the wavelength range 3.8-6.1 \AA\ during solar flares. The fluxes are analyzed to give the sulphur abundance.…

Solar and Stellar Astrophysics · Physics 2015-06-04 J. Sylwester , B. Sylwester , K. J. H. Phillips , V. D. Kuznetsov

Coronal plumes are bright, narrow structures rooted in coronal holes that contribute to the solar wind. Their composition, particularly elemental fractionation as a function of first ionization potential (FIP), provides diagnostics of…

Solar and Stellar Astrophysics · Physics 2026-02-27 Slimane Mzerguat , Miho Janvier , Eric Buchlin , Deborah Baker , Andy S. H. To , David M. Long , Natalia Zambrana Prado

The RS CVn binary system HR 1099 was extensively observed by the XMM-Newton observatory in February 2000 as its first-light target. A total of 570 ks of exposure time was accumulated with the Reflection Grating Spectrometers (RGS). The…

Radiative losses play a critical role in the cooling of plasmas. When chromospheric plasma is sufficiently heated, it can flow into coronal loops which subsequently cool down due to radiation. From observations, we infer that this cooling…

Solar and Stellar Astrophysics · Physics 2025-09-16 Luke Fushimi Benavitz , Jeffrey W. Reep , Lucas A. Tarr , Andy S. H. To

Following the Chandra Orion Ultradeep Project (COUP) observation, we have studied the chemical composition of the hot plasma in a sample of 146 X-ray bright pre-main sequence stars in the Orion Nebula Cluster. We report measurements of…

Astrophysics · Physics 2011-02-11 A. Maggio , E. Flaccomio , F. Favata , G. Micela , S. Sciortino , E. D. Feigelson , K. V. Getman

A model for element abundance fractionation between the solar chromosphere and corona is further developed. The ponderomotive force due to Alfven waves propagating through, or reflecting from the chromosphere in solar conditions generally…

Solar and Stellar Astrophysics · Physics 2015-05-30 J. Martin Laming

IIPeg is an ideal target to study stellar activity and flares, since intense and long lasting flares have been frequently detected from this system at all wavelengths. We report here about a BeppoSAX observation of IIPeg. We followed the…

Astrophysics · Physics 2007-05-23 S. Covino , G. Tagliaferri , R. Pallavicini , R. Mewe , E. Poretti

Plasma composition measurements are a vital tool for the success of current and future solar missions, but density and temperature insensitive spectroscopic diagnostic ratios are sparse, and their underlying accuracy in determining the…

Solar and Stellar Astrophysics · Physics 2024-10-22 David H. Brooks , Harry P. Warren , Deborah Baker , Sarah A. Matthews , Stephanie L. Yardley

Sun-as-a-star coronal plasma composition, derived from full-Sun spectra, and the F10.7 radio flux (2.8 GHz) have been shown to be highly correlated (r = 0.88) during solar cycle 24. However, this correlation becomes nonlinear during…

$\beta$ Cet, 31 Com and $\mu$ Vel represent the main stages through which late-type giants evolve during their lifetime (the Hertzsprung gap (31 Com), the rapid braking zone ($\mu$ Vel) and the core helium burning ``clump'' phase ($\beta$…

Astrophysics · Physics 2009-11-13 D. Garcia-Alvarez , J. J. Drake , B. Ball , L. Lin , V. L. Kashyap

Ponderomotive acceleration has been asserted to be a cause of the First Ionization Potential (FIP) effect, the by now well known enhancement in abundance by a factor of 3-4 over photospheric values of elements in the solar corona with FIP…

Solar and Stellar Astrophysics · Physics 2016-11-15 R. B. Dahlburg , J. M. Laming , B. D. Taylor , K. Obenschain