中文
相关论文

相关论文: Coronal Elemental Abundances in Solar Emerging Flu…

200 篇论文

We revisit in more detail a model for element abundance fractionation in the solar chromosphere, that gives rise to the "FIP Effect" in the solar corona and wind. Elements with first ionization potential below about 10 eV, i.e. those that…

太阳与恒星天体物理 · 物理学 2014-11-18 J. Martin Laming

We find that the element abundances in solar energetic particles (SEPs) and in the slow solar wind (SSW), relative to those in the photosphere, show different patterns as a function of the first ionization potential (FIP) of the elements.…

太阳与恒星天体物理 · 物理学 2018-03-13 Donald V. Reames

Elemental abundance effects in active coronae have eluded our understanding for almost three decades, since the discovery of the First Ionization Potential (FIP) effect on the sun. The goal of this paper is to monitor the same coronal…

太阳与恒星天体物理 · 物理学 2012-12-04 Raanan Nordon , Ehud Behar , Stephen A. Drake

We investigate the time evolution of relative elemental abundances in the context of the first ionization potential effect focusing on an active region. Our aim is to characterize this evolution in different types of solar active region…

太阳与恒星天体物理 · 物理学 2026-02-11 T. Varesano , D. M. Hassler , N. Zambrana Prado , J. M. Laming , J. Plowman , D. J. Knipp , M. Molnar , K. Barczynski , The SPICE consortium

Within the coronae of stars, abundances of those elements with low first ionization potential (FIP) often differ from their photospheric values. The coronae of the Sun and solar-type stars mostly show enhancements of low-FIP elements (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…

太阳与恒星天体物理 · 物理学 2025-09-16 Luke Fushimi Benavitz , Jeffrey W. Reep , Lucas A. Tarr , Andy S. H. To

The different elemental abundances of the photosphere and the corona are striking features of not only the Sun, but other stars as well. This phenomenon is known as the FIP effect (FIP stands for first ionization potential), and its…

太阳与恒星天体物理 · 物理学 2022-03-14 B. Seli , K. Oláh , L. Kriskovics , Zs. Kővári , K. Vida , L. G. Balázs , J. M. Laming , L. van Driel-Gesztelyi , D. Baker

Solar atmospheric elemental abundances are now known to vary both in space and time. Dynamic modeling of these changes is therefore necessary to improve the accuracy of radiative hydrodynamic simulations. Recent studies have shown that…

太阳与恒星天体物理 · 物理学 2026-02-13 David H. Brooks , Jeffrey W. Reep , Andy S. H. To , Luke Fushimi Benavitz , Lucas A. Tarr

Plasma composition in the solar corona commonly differs from that of the photosphere, with the enhancement of low--first-ionization-potential (FIP) elements referred to as the FIP effect. This phenomenon provides important diagnostics of…

太阳与恒星天体物理 · 物理学 2026-03-25 Man-Hei Ng , Xiaoping Zhang , P. F. Chen

The composition of the solar corona differs from that of the photosphere, with the plasma thought to fractionate in the solar chromosphere according to the First Ionisation Potential (FIP) of the different elements. This produces a FIP…

Elemental abundances in the solar corona differ from those in the photosphere, with low first ionization potential (FIP) elements being enhanced, a phenomenon known as the FIP effect. This enhancement is attributed to ponderomotive forces…

太阳与恒星天体物理 · 物理学 2025-04-23 Kyoung-Sun Lee , Jongchul Chae , Hannah Kwak , Kyuhyoun Cho , Kyeore Lee , Juhyung Kang , Eun-Kyung Lim , Donguk Song

The Inverse First Ionization Potential (FIP) Effect, the depletion in coronal abundance of elements like Fe, Mg, and Si that are ionized in the solar chromosphere relative to those that are neutral, has been identified in several solar…

太阳与恒星天体物理 · 物理学 2021-03-17 J. Martin Laming

The Solar First Ionization Potential (FIP) effect, where low-FIP elements are enriched in the corona relative to the photosphere, while high-FIP abundances remain unchanged, has been known for a long while. High resolution X-ray…

天体物理学 · 物理学 2009-11-13 R. Nordon , E. Behar

Coronal elemental abundances are known to deviate from the photospheric values of their parent star, with the degree of deviation depending on the First Ionization Potential (FIP). This study focuses on the coronal composition of stars with…

太阳与恒星天体物理 · 物理学 2015-05-13 Uria Peretz , Ehud Behar , Stephen A. Drake

We present evidences that anomalies in abundance of the chemical minor elements with the low first ionization potential (FIP) in the low corona of the late-type stars can be related with topology of the large-scale magnetic field. The solar…

太阳与恒星天体物理 · 物理学 2018-05-09 V. V. Pipin , V. M. Tomozov

We present measurements of relative elemental abundances in plumes and interplumes. Plumes are bright, narrow structures in coronal holes that extend along open magnetic field lines far out into the corona. Previous work has found that in…

太阳与恒星天体物理 · 物理学 2015-07-15 Chloé Guennou , Michael Hahn , Daniel Wolf Savin

Context. Elemental abundances in some coronal structures differ significantly from photospheric abundances, with a dependence on the first ionization potential (FIP) of the element. Measuring these FIP-dependent abundance biases is…

太阳与恒星天体物理 · 物理学 2019-11-26 Natalia Zambrana Prado , Éric Buchlin

From a turbulent history, the study of abundances of elements in solar energetic particles (SEPs) has grown into an extensive field that probes the solar corona and the physical processes of SEP acceleration and transport. Underlying SEPs…

太阳与恒星天体物理 · 物理学 2019-11-22 Donald V Reames

We have used Chandra to resolve the nearby 70 Oph (K0 V+K5 V) and 36 Oph (K1 V+K1 V) binary systems for the first time in X-rays. The LETG/HRC-S spectra of all four of these stars are presented and compared with an archival LETG spectrum of…

天体物理学 · 物理学 2009-11-11 Brian E. Wood , Jeffrey L. Linsky

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…