The Effects of Transverse Magnetic Field and Density Variations on the Particle Energy Spectra in a Reconnecting 3D Current Sheet

• DOI: 10.1007/s11214-006-6027-7
• Publication Date: 2006-06-01T22:58:22Z
• Authors: Valentina V. Zhar...; Mykola Gordovskyy
• Keywords: Spectral index; Current sheet; Exponent

Electron and proton acceleration by a super-Dreicer electric field is further investigated in a non-neutral reconnecting current sheet (RCS) with a variable plasma density. The tangential Bz and transverse magnetic field components Bx are assumed to vary with the distances x and z from the X nullpoint linearly and exponentially, respectively; the longitudinal component (a ‘guiding field’) is accepted constant. Particles are found to gain a bulk of their energy in a thin region close to the X nullpoint where the RCS density increases with z exponentially with the index λ and the tangential magnetic field Bx also increases with z exponentially with the index α. For the RCS with a constant density (λ = 0), the variations of the tangential magnetic field lead to particle power-law energy spectra with the spectral indices γ1 being dependent on the exponent α as: \(\gamma_1 = 1 + \frac{1}{2\alpha}\) for protons and \(\gamma_1 = 1+ \frac{1}{\alpha}\) for electrons in a strong guiding field (β > 10−2) and \(\gamma_1 =\frac {1} 2 (1 +\frac{1}{\alpha})\) for electrons in a moderate or weak guiding field (β > 10−4). For the RCS with an exponential density increase in the vicinity of the X nullpoint (λ≥ 0) there is a further increase of the resulting spectral indices γ that depends on the density exponent index λ as \(\gamma = \gamma_1 +\frac{\lambda}{2\alpha}\) for protons and for electrons in weaker guiding fields and as \(\gamma = \gamma_1 + \frac{\lambda}{\alpha}\) for electrons in stronger guiding fields. These dependencies can explain a wide variety (1.5–10) of particle spectral indices observed in solar flares by the variations of a magnetic field topology and physical conditions in a reconnecting region. This can be used as a diagnostic tool for the investigation of the RCS dynamics from the accelerated particle spectra found from hard X-ray and microwave emission.