Hostname: page-component-8448b6f56d-wq2xx Total loading time: 0 Render date: 2024-04-16T18:15:42.388Z Has data issue: false hasContentIssue false

Energetic Particles in a Flare Loop: Spectra and Radiation Signatures

Published online by Cambridge University Press:  19 July 2016

P. A. Bespalov
Affiliation:
Institute of Applied Physics Gorky, USSR
V. V. Zaitsev
Affiliation:
Institute of Applied Physics Gorky, USSR
A. V. Stepanov
Affiliation:
Crimean Astrophysical Observatory Crimea, USSR

Abstract

Core share and HTML view are not available for this content. However, as you have access to this content, a full PDF is available via the ‘Save PDF’ action button.

It has been shown that high energy particle spectra, particle dynamics, and radiation in a flare loop are determined by wave-particle interactions. The electron-whistler interaction occurs under conditions of strong pitch angle diffusion that makes the particle distribution function isotropic. The flare loop electrons retain information about the particle source spectrum. The interaction of energetic ions with Alfven waves is characterized by strong, moderate, and weak diffusion. The time delays in hard X-ray and gamma-ray emission during one-step acceleration processes might be understood in terms of a trap-plus-turbulent propagation model. The density of precipitating particles is less than or equal to the trapping one. Radiation signatures of flare loop electrons are discussed.

Type
VIII. Solar Flares
Copyright
Copyright © Kluwer 1990 

References

REFERENCES

Aschwander, M.J., Benz, A.O. and Kane, S.R. (1989) “Correlation of solar radio pulsations with hard X-ray emission”, Astron. Astrophys. in press.Google Scholar
Bai, T. and Ramaty, R. (1979) “Hard X-ray time profiles and acceleration processes in large solar flares”, Ap. J., 227, 10721081.Google Scholar
Bespalov, P.A. and Trakhtengertz, V. Yu. (1986) “Cyclotron instability in the Earth radiation belts”, in Reviews of Plasma Physics, vol. 10, Plenum Publ. Corp., New York.Google Scholar
Bespalov, P.A. and Zaitsev, V.V. (1986) “Formation of energetic proton spectra in solar flares” in Solar Maximum Analysis, VNU Sci. Press, p.247253.Google Scholar
Bespalov, P.A., Zaitsev, V.V. and Stepanov, A.V. (1987) “On the origin of time delays in hard X-ray and gamma-ray emission of solar flares”, Solar Phys. 114, 127140.Google Scholar
Bespalov, P.A., Zaitsev, V.V. and Stepanov, A.V. (1990) “Consequences of strong pitch angle diffusion of particles in solar flares”, Ap.J. Suppl. in press.Google Scholar
Blanken, R.A. and Kuckes, A.F. (1969) “Synchrotron deceleration of electrons in plasma and the generation of electromagnetic radiation” Plasma Phys. 11, 321331.CrossRefGoogle Scholar
Chupp, E.L. (1983) “High energy particle acceleration in solar flares - observational evidence”, Solar Phys., 86, 383393.Google Scholar
Gary, D.E. (1985) “The numbers of fast electrons in solar flares as deduced from hard X-ray and microwave spectral data”, Ap.J., 297, 799804.Google Scholar
Hulot, E., Vilmer, N. and Trottet, G. (1989) “Relative timing of solar prompt gamma-ray line and X-ray emission expected from a trap plus precipitation model for protons and electrons”, Astron. Astrophys., 213, 383396.Google Scholar
Kai, K. (1982) “An explanation of discrepancy of required electron numbers between concurrent mcw and hard X-ray bursts”, in Hinotori Symposium on Solar Flares, Tokyo, pp. 162167.Google Scholar
Kennel, C.F. and Petschek, H.E. (1966) “Limit of stability trapped particle fluxes”, J. Geophys. Res. 71, 122.CrossRefGoogle Scholar
Melrose, D.B. and Brown, J.C. (1976) “Precipitation in trap models for solar hard X-ray bursts”, Mon. Not. R.A.S. 176, 1530.Google Scholar
Zweibel, E.G. and Haber, D.A. (1983) “The propagation of energetic ions in magnetic loops and gamma-ray emission from solar flares”, Ap. J., 264, 648659.CrossRefGoogle Scholar