Dynamic models of optical emission in impulsive solar flares

Citation
Wp. Abbet et Sl. Hawley, Dynamic models of optical emission in impulsive solar flares, ASTROPHYS J, 521(2), 1999, pp. 906-919
Citations number
47
Categorie Soggetti
Space Sciences
Journal title
ASTROPHYSICAL JOURNAL
ISSN journal
0004637X → ACNP
Volume
521
Issue
2
Year of publication
1999
Part
1
Pages
906 - 919
Database
ISI
SICI code
0004-637X(19990820)521:2<906:DMOOEI>2.0.ZU;2-F
Abstract
Numerical simulations of the dynamics and radiation in a solar hare loop ar e presented. The heating processes in the lower atmosphere include nontherm al heating by accelerated electrons and thermal soft X-ray irradiation from the flare-heated transition region and corona. Important transitions of hy drogen, helium, and singly ionized calcium and magnesium are treated in non -LTE. The principal results of the analysis are the following: 1. An impulsive event can be described as having two distinct dynamic phase s, each with a definite observational signature: an initial gentle phase, c haracterized by an atmospheric state of near-equilibrium, and a subsequent explosive phase, characterized by large material flows and strong hydrodyna mic waves and shocks. The amount of time the atmosphere remains in the gent le phase is determined by the level of nonthermal heating. Excess line emis sion produced during the gentle phase is not significantly Doppler-shifted, and the profiles remain symmetric about their nominal line-center frequenc ies. Emission profiles generated during the explosive phase can be highly D oppler-shifted and distorted, reflecting the material motion and steep velo city gradients present at their depths of formation. 2. Hydrogen recombination radiation, from a high-temperature plateau formed during the gentle phase and from a chromospheric condensation formed durin g the explosive phase, is the primary cause of the white-light continuum br ightening produced in the simulations. 3. A time lag is found between the brightening of the Paschen continuum and the brightening of the near wings of Ha, in the sense that the line wings brighten immediately, but the continuum first undergoes a slight dimming, f ollowed eventually by a brightening. The continuum behavior is controlled b y the trade-off between increased photoionization from enhanced populations of the excited states of hydrogen and increased electron density, which pr omotes recombination. 4. During the impulsive phase, when the accelerated electrons are directly heating the upper chromosphere, the contribution of the thermal soft X-rays to the overall energy balance in the lower atmosphere is negligible.