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PIC code simulations of solar flare processes Astronomical Institute

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1 PIC code simulations of solar flare processes Astronomical Institute
Marian Karlický Miroslav Bárta Dieter Nickeler Astronomical Institute Ondřejov Czech Republic

2 Contents: 2. Tearing and coalescence processes in
1. Introduction to solar flare theory 2. Tearing and coalescence processes in the current sheet (2.5-D PIC model) Drifting pulsation structures 3. Fragmentation of the current sheet (3-D PIC model) 4. Spatial separation of accelerated particles in magnetic reconnection 5. Return current simulations (3-D PIC model) 6. Conclusions

3 CME-flare phenomenon Forbes and Acton 1996, ApJ 459, 330
Lin and Forbes 2000, JGR 105, 2375

4 Particle-in-cell simulations:

5 Particle-in-cell simulations:
Drake et al. 2005, Phys. Rev. Lett. 94, Pritchett 2006, J. Geophys. Res. 111, A10212 Karlický and Bárta 2007, AA 464, 735 2.5 D electromagnetic relativistic PIC code (Saito, Sakai: 2004, ApJ 616, L179) Numerical box 2000x600 grids Current sheet, half-width 10 grids Parallel code, Ondřejov Cluster for Astrophysical Simulations

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11 July 11, 2002

12 Current sheet fragmentation
3D PIC model (Karlický and Bárta, 2007) 25x105x805 grids, 2 current sheets, periodic boundary conditions, guiding field Bz=5xB0, mi/me=1836, wce/wpe=0.2 Times: wpet = 0, 250, 500, 750 See also Jaroschek et al. 2004, Phys. Plasmas 11, 1151

13 Times: wpet = 0, 250, 500, 750 Resulting ratio of resistivities ha/hC ~ 105

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15 Separation of accelerated electrons and positrons
in the relativistic reconnection electrons positrons Separation of electrons and protons in RHESSI observations of the July 23, 2002 flare (Hurford et al. 2003)

16 Return current simulations
Motivation: Bombardment of the chromosphere by electron beams. Effects in intensities and polarization of the optical chromospheric lines during solar flares (Karlický et al. 2004, AA 416, L13). Model: 3-D PIC (Buneman 1993) 5x5x800 mi/me=1836, Te= 105 and 104 K, vb/c = 0.36, nb/ne = 1.66x10-2 and 1.66x10-3 (transition region and chromoshere) (20/1200 and 20/12000 particles per cube)

17 Electron distribution functions
Times: wpet = 0, 100, 250, 2500 (TR)

18 The time evolution of electric field energy (TR)

19 The time evolution of total electric current (TR)

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21 Electron distribution functions
Times: wpet = 0, 1250, 2500, 5000 (CHR)

22 The energy electron distribution function
In the chromoshere without (left) and with (right) electron beam and return current

23 Conclusions: The PIC models show that the current sheets are unstable due to tearing mode instability and they become very fragmented due to Buneman and kinetic kink instability. These processes support fast dissipation of the magnetic field energy. Magnetic reconnection with the guiding magnetic field spatially separates particles. 3. Observational evidence of these processes is: moving plasmoids, radio drifting pulsation structures, evolving X-ray and radio loop-top sources. A formation of the return current is presented. This current is formed by electrons from the bulk as well as from the tail of the distribution function. Resuls are very important for computations of intensities and polarization of optical chromospheric lines.


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