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Energy Transport and Heating by Non-Thermal Electrons in a Turbulent Solar Flare Environment

A. Gordon Emslie, Eduard P. Kontar

Abstract

The impulsive phase of a solar flare is known to generate strong turbulence and to transfer magnetic energy into accelerated electrons. Recognizing the importance of angular diffusion on the dynamics of the accelerated electrons, we extend previous treatments by deriving analytic solutions for the electron flux and associated energy deposition in two regimes: scattering dominated by inelastic Coulomb collisions and scattering dominated by elastic interactions with turbulent scattering centers. We show that the turbulence-dominated scattering term strongly reshapes the spatial distribution of the plasma heating: compared to the traditional collisional thick-target approach, turbulent scattering could lead to an order-of-magnitude increase in coronal heating and an even greater suppression of chromospheric heating. Scattering also acts to reduce the anisotropy of the electron distribution and so reduces the net current associated with the nonthermal electrons. The return-current Ohmic heating is accordingly reduced to a level that renders it negligible compared to direct collisional heating. The results have significant implications for models of atmospheric response to impulsive phase energy release, in particular chromospheric evaporation, flare-driven coronal heating, the formation of loop-top hard X-ray sources, and the longstanding discrepancy between modeled and observed soft X-ray line profiles.

Energy Transport and Heating by Non-Thermal Electrons in a Turbulent Solar Flare Environment

Abstract

The impulsive phase of a solar flare is known to generate strong turbulence and to transfer magnetic energy into accelerated electrons. Recognizing the importance of angular diffusion on the dynamics of the accelerated electrons, we extend previous treatments by deriving analytic solutions for the electron flux and associated energy deposition in two regimes: scattering dominated by inelastic Coulomb collisions and scattering dominated by elastic interactions with turbulent scattering centers. We show that the turbulence-dominated scattering term strongly reshapes the spatial distribution of the plasma heating: compared to the traditional collisional thick-target approach, turbulent scattering could lead to an order-of-magnitude increase in coronal heating and an even greater suppression of chromospheric heating. Scattering also acts to reduce the anisotropy of the electron distribution and so reduces the net current associated with the nonthermal electrons. The return-current Ohmic heating is accordingly reduced to a level that renders it negligible compared to direct collisional heating. The results have significant implications for models of atmospheric response to impulsive phase energy release, in particular chromospheric evaporation, flare-driven coronal heating, the formation of loop-top hard X-ray sources, and the longstanding discrepancy between modeled and observed soft X-ray line profiles.

Paper Structure

This paper contains 7 sections, 20 equations, 4 figures.

Figures (4)

  • Figure 1: Energy flux ${\cal F}(z)$ vs. distance $z$ from the (loop top) acceleration region. The solid line shows the results for collisional scattering, with the dashed line showing the behavior in the non-diffusive approach. The other lines show the results for turbulent scattering, with a turbulent scattering length $\lambda_T$ equal to $0.1 \times$ (red), $0.2 \times$ (green), and $0.3 \times$ (blue) the collisional mean free path of $7 \times 10^7$ cm.
  • Figure 2: Collisional heating rate $Q$ vs. distance from the (loop top) acceleration region. The solid line shows the results for collisional scattering, with the dashed line showing the behavior in the non-diffusive approach. The other lines show the results for turbulent scattering, with a turbulent scattering length $\lambda_T$ equal to $0.1 \times$ (red), $0.2 \times$ (green), and $0.3 \times$ (blue) the collisional mean free path of $7 \times 10^7$ cm.
  • Figure 3: Ohmic heating rate $Q_{rc}$ vs. distance from the (loop top) acceleration region. The solid line shows the results for collisional scattering, and the other lines show the results for turbulent scattering, with a turbulent scattering length $\lambda_T$ equal to $0.1 \times$ (red), $0.2 \times$ (green), and $0.3 \times$ (blue) the collisional mean free path of $7 \times 10^7$ cm. (Note that the abscissa is now on a logarithmic scale.)
  • Figure 4: Ratio of Ohmic to collisional heating $Q_{rc}/Q$. The solid line shows the results for collisional scattering, and the other lines show the results for turbulent scattering, with a turbulent scattering length $\lambda_T$ equal to $0.1 \times$ (red), $0.2 \times$ (green), and $0.3 \times$ (blue) the collisional mean free path of $7 \times 10^7$ cm. The ratio is $\ll 1$ at all positions in the target in all cases.