Solar Microwave Bursts and Injection Pitch-Angle Distribution of Flare Electrons

We calculate the time variation of the energy and pitch angle of high-energy electrons injected into a magnetic loop and subsequently trapped there because of magnetic mirroring. We use the evolving distribution in the calculation of gyrosynchrotron emission, as an aid to interpretation of a particular microwave burst observed using the Owens Valley Solar Array (OVSA) during a GOES class C2.8 flare on 1993 June 3. The electrons are assumed to have a Gaussian pitch-angle distribution, whose width and mean pitch angle are calculated as they evolve in time, taking into account the electron energy loss and a specific magnetic loop structure set as a model for the target active region. Various temporal behaviors of the microwave spectrum are found as a function of injection and trap conditions, which can be used to infer some of the injection properties directly from the observed microwave spectra. As a main result we found that initial pitch-angle distribution plays an important role in the microwave spectral evolution. This is largely due to the fact that pitch-angle diffusion of electrons under Coulomb collisions markedly differs at those electron energies to which the microwave spectrum is sensitive. This effect cannot be reproduced by adjusting the trap properties and therefore could be used to determine whether the initial pitch-angle distribution is isotropic or narrowly beamed. The microwave burst spectra observed during the 1993 June 3 flare are found to be most consistent with the hypothesis of an initially narrow beamed injection (≤30°) into a low-density (~4 × 109 cm-3) magnetic trap. This result explains the observed asymmetric microwave time curve consisting of a relatively short rise (~32 s) and a long decay (≥5 minutes) in terms of a transport effect rather than acceleration characteristics. The physical connection of the proposed microwave model to hard X-ray models in thin/thick targets is briefly discussed.

[1]  M. Kundu,et al.  Observations and Models of a Flaring Loop , 2000 .

[2]  K. Shibasaki,et al.  Magnetic Trapping and Electron Injection in Two Contrasting Solar Microwave Bursts , 2000 .

[3]  L. Fletcher,et al.  A Model for Hard X-Ray Emission from the Top of Flaring Loops , 1998 .

[4]  Markus J. Aschwanden,et al.  Deconvolution of Directly Precipitating and Trap-Precipitating Electrons in Solar Flare Hard X-Rays. I. Method and Tests , 1998 .

[5]  M. Aschwanden,et al.  Electron Trapping Times and Trap Densities in Solar Flare Loops Measured with COMPTON and YOHKOH , 1997 .

[6]  Takeo Kosugi,et al.  Electron Time-of-Flight Distances and Flare Loop Geometries Compared from CGRO and YOHKOH Observations , 1996 .

[7]  J. McTiernan,et al.  Gamma-ray emission and electron acceleration in solar flares , 1994 .

[8]  V. Mel’nikov Electron acceleration and capture in impulsive and gradual bursts: Results of analysis of microwave and hard x-ray emissions , 1994 .

[9]  N. Vilmer,et al.  Electron trapping in evolving coronal structures during a large gradual hard X-ray/radio burst , 1994 .

[10]  J. McTiernan,et al.  The Behavior of Beams of Relativistic Nonthermal Electrons under the Influence of Collisions and Synchrotron Losses , 1990 .

[11]  E. Lu,et al.  Numerical solution of the time-dependent kinetic equation for electrons in magnetized plasma , 1990 .

[12]  James A. Miller,et al.  Relativistic electron transport and bremsstrahlung production in solar flares , 1989 .

[13]  M. Kundu,et al.  Simultaneous multi-frequency imaging observations of solar microwave bursts , 1989 .

[14]  E. Lu,et al.  Rapid Temporal Evolution of Radiation from Nonthermal Electrons in Solar Flares , 1988 .

[15]  K. Klein,et al.  Microwave diagnostics of energetic electrons in flares , 1986 .

[16]  D. Gary,et al.  An impulsive solar burst observed in H-alpha, microwaves, and hard X-rays , 1985 .

[17]  J. Leach,et al.  The impulsive phase of solar flares. II - Characteristics of the hard X-rays , 1983 .

[18]  K. A. Marsh,et al.  Simplified expressions for the gyrosynchrotron radiation from mildly relativistic, nonthermal and thermal electrons , 1982 .

[19]  T. Bai Transport of energetic electrons in a fully ionized hydrogen plasma. [in solar flares] , 1982 .

[20]  V. Petrosian Synchrotron emissivity from mildly relativistic particles , 1981 .

[21]  V. Petrosian,et al.  Impulsive phase of solar flares. 1: Characteristics of high energy electrons , 1981 .

[22]  R. Ramaty,et al.  Hard X-ray time profiles and acceleration processes in large solar flares , 1979 .

[23]  Effect of Asymmetry on a Trap Model for Solar Hard Xray Bursts , 1979 .

[24]  J. Brown,et al.  Precipitation in Trap Models for Solar Hard X-ray Bursts , 1976 .

[25]  R. Gould Energy loss of fast electrons and positrons in a plasma , 1972 .

[26]  R. Ramaty Gyrosynchrotron emission and absorption in a magnetoactive plasma , 1969 .

[27]  Charles F. Kennel,et al.  Consequences of a magnetospheric plasma , 1969 .