Search results for "Coronal radiative losses"

showing 5 items of 5 documents

Evidence of nonthermal particles in coronal loops heated impulsively by nanoflares

2014

The physical processes causing energy exchange between the Sun's hot corona and its cool lower atmosphere remain poorly understood. The chromosphere and transition region (TR) form an interface region between the surface and the corona that is highly sensitive to the coronal heating mechanism. High resolution observations with the Interface Region Imaging Spectrograph (IRIS) reveal rapid variability (about 20 to 60 seconds) of intensity and velocity on small spatial scales at the footpoints of hot dynamic coronal loops. The observations are consistent with numerical simulations of heating by beams of non-thermal electrons, which are generated in small impulsive heating events called "corona…

High Energy Astrophysical Phenomena (astro-ph.HE)PhysicsMultidisciplinaryFOS: Physical sciencesCoronal holeCoronal loopElectronAstrophysicsCoronaCoronal radiative losses3. Good healthNanoflaresAtmosphereSettore FIS/05 - Astronomia E AstrofisicaAstrophysics - Solar and Stellar Astrophysics13. Climate actionPhysics::Space PhysicsAstrophysics::Solar and Stellar AstrophysicsAstrophysics - High Energy Astrophysical PhenomenaChromosphereSolar and Stellar Astrophysics (astro-ph.SR)Science
researchProduct

The Sun as an X‐Ray Star. IV. The Contribution of Different Regions of the Corona to Its X‐Ray Spectrum

2001

We study X-ray-synthesized spectra of solar regions as templates to interpret analogous stellar spectra. We define three classes of coronal structures of different brightness, low (background quiet corona), medium (active regions), and high (active region cores), and determine their contribution to the solar X-ray emission measure versus temperature, EM(T), luminosity, and spectrum. This study defines the extent of the solar analogy quantitatively and accurately. To this end, we have selected a large sample of full-disk Yohkoh soft X-ray telescope observations taken between the maximum and the minimum of solar cycle 22, obtaining the contribution of each class to the whole Sun's EM(T). From…

PhysicsAstrophysics::High Energy Astrophysical PhenomenaAstronomyAstronomy and AstrophysicsSolar cycle 22AstrophysicsCoronal loopCoronaCoronal radiative lossesAstronomical spectroscopyLuminosityStarsSpace and Planetary SciencePhysics::Space PhysicsROSATAstrophysics::Solar and Stellar AstrophysicsAstrophysics::Earth and Planetary AstrophysicsThe Astrophysical Journal
researchProduct

The Corona of the Sun as a Star

2006

We study the physics of the solar corona as a whole, i.e. of the Sun as a Star, in order to understand its global features and to provide a template for stellar coronae. In this process we strive to understand the features of various structures which compose the solar corona. This process in not straightforward given the problems of observing the Sun as a whole: e.g., no recent X‐ray wide‐band, medium‐resolution, spectrum of the Sun is avaible, unlike stars and no X‐ray spectral monitoring of the Sun at various activity phases is available. The presentation will discuss our work in this field; we present the method we have devised, based on Yohkoh/SXT data, to derive the Differential Emissi…

PhysicsField (physics)Astrophysics::High Energy Astrophysical PhenomenaStellar atmosphereAstronomyA* search algorithmAstrophysicsCoronal radiative lossesCoronaCorona X-ray and gamma-ray emission X-raylaw.inventionStarsSettore FIS/05 - Astronomia E AstrofisicalawPhysics::Space PhysicsCoronal heatingAstrophysics::Solar and Stellar AstrophysicsAstrophysics::Earth and Planetary AstrophysicsX ray spectra
researchProduct

The Sun as a benchmark of flaring activity in stellar coronae

2009

The solar corona is a template to study and understand stellar activity. However the solar corona differs from that of active stars: the Sun has lower X‐ray luminosity, and on average cooler plasma temperatures. Active stellar coronae have a hot peak in their emission measure distribution, EM (T), at 8–20 MK, while the non‐flaring solar corona has a peak at 1–2 MK. In the solar corona significant amounts of plasma at temperature ∼10 MK are observed only during flares.To investigate what is the time‐averaged effect of solar flares we measure the disk‐integrated time‐averaged emission measure, EMF (T), of an unbiased sample of solar flares. To this aim we analyze uninterrupted GOES/XRS light …

PhysicsSolar flareStar formationopacity and line formationAstronomyStellar atmospheresAstrophysicsCoronal loopCoronal radiative lossesCoronalaw.inventionSolar cycleNanoflaresSettore FIS/05 - Astronomia E Astrofisicaradiative transferlawCoronal mass ejectionX-ray emission spectra and fluorescence gamma-rayFlareAIP Conference Proceedings
researchProduct

Coronal Magnetic Field Measurements Through Quasi-Transverse Propagation

2004

The QT-propagation of microwaves as a means to measure coronal magnetic fields and the inversion of circular polarization as an observational proof of the QT-propagation are discussed. The first part of the chapter briefly outlines the relevant geometry and mathematical relations. Then the state of the art in the coronal magnetography and some possibilities are demonstrated. We discuss use of the technique for coronal magnetography and give some estimates concerning the coronal magnetography with the forthcoming Frequency Agile Solar Radiotelescope.

PhysicsTransverse planeSolar windPhysics::Space PhysicsStellar magnetic fieldAstrophysics::Solar and Stellar AstrophysicsAstronomyMagnetic reconnectionCoronal loopCoronaCoronal radiative lossesComputational physicsNanoflares
researchProduct