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Title: Particle Acceleration during Magnetic Reconnection in a Low-beta Plasma

Abstract

Magnetic reconnection is a primary mechanism for particle energization in space and astrophysical plasmas. By carrying out two-dimensional (2D) fully kinetic simulations, we study particle acceleration during magnetic reconnection in plasmas with different plasma β (the ratio between the thermal pressure and the magnetic pressure). For the high-β cases, we do not observe significant particle acceleration. In the low-β regime ($$\beta \lt 0.1$$), we find that reconnection is efficient at energizing both electrons and ions. While the distribution of accelerated particles integrated over the whole simulation box appears highly non-thermal, it is actually the superposition of a series of distributions in different sectors of a 2D magnetic island. Each of those distributions has only a small non-thermal component compared with its thermal core. By tracking a large number of particles, we show that particles get energized in X-line regions, contracting magnetic islands, and magnetic island coalescence regions. We obtain the particle energization rate $${\boldsymbol{j}}\cdot {\boldsymbol{E}}$$ by averaging over particle drift motions and find that it agrees well with the particle kinetic energy change. We quantify the contribution of curvature drift, gradient drift, polarization drift, magnetization, non-gyrotropic effect, and parallel electric field in different acceleration regions. We find that the major energization is due to particle curvature drift along the motional electric field. The other particle motions contribute less but may become important in different acceleration regions. The highly efficient particle energization in low-β plasmas may help us understand the strong particle energization in solar flares and accretion disk coronae.

Authors:
ORCiD logo [1]; ORCiD logo [2]; ORCiD logo [2]; ORCiD logo [3]
  1. Univ. of Alabama, Huntsville, AL (United States). Dept. of Space Science; Univ. of Alabama, Huntsville, AL (United States). Center for Space Plasma and Aeronomic Research; Los Alamos National Lab., Los Alamos, NM (United States)
  2. Los Alamos National Lab. (LANL), Los Alamos, NM (United States)
  3. Univ. of Alabama, Huntsville, AL (United States). Dept. of Space Science
Publication Date:
Research Org.:
Lawrence Berkeley National Laboratory (LBNL), Berkeley, CA (United States). National Energy Research Scientific Computing Center (NERSC)
Sponsoring Org.:
USDOE
OSTI Identifier:
1524226
Resource Type:
Accepted Manuscript
Journal Name:
The Astrophysical Journal (Online)
Additional Journal Information:
Journal Name: The Astrophysical Journal (Online); Journal Volume: 843; Journal Issue: 1; Journal ID: ISSN 1538-4357
Publisher:
Institute of Physics (IOP)
Country of Publication:
United States
Language:
English
Subject:
79 ASTRONOMY AND ASTROPHYSICS; acceleration of particles; accretion; accretion disks; magnetic reconnection; Sun: corona; Sun: flares

Citation Formats

Li, Xiaocan, Guo, Fan, Li, Hui, and Li, Gang. Particle Acceleration during Magnetic Reconnection in a Low-beta Plasma. United States: N. p., 2017. Web. doi:10.3847/1538-4357/aa745e.
Li, Xiaocan, Guo, Fan, Li, Hui, & Li, Gang. Particle Acceleration during Magnetic Reconnection in a Low-beta Plasma. United States. https://doi.org/10.3847/1538-4357/aa745e
Li, Xiaocan, Guo, Fan, Li, Hui, and Li, Gang. Tue . "Particle Acceleration during Magnetic Reconnection in a Low-beta Plasma". United States. https://doi.org/10.3847/1538-4357/aa745e. https://www.osti.gov/servlets/purl/1524226.
@article{osti_1524226,
title = {Particle Acceleration during Magnetic Reconnection in a Low-beta Plasma},
author = {Li, Xiaocan and Guo, Fan and Li, Hui and Li, Gang},
abstractNote = {Magnetic reconnection is a primary mechanism for particle energization in space and astrophysical plasmas. By carrying out two-dimensional (2D) fully kinetic simulations, we study particle acceleration during magnetic reconnection in plasmas with different plasma β (the ratio between the thermal pressure and the magnetic pressure). For the high-β cases, we do not observe significant particle acceleration. In the low-β regime ($\beta \lt 0.1$), we find that reconnection is efficient at energizing both electrons and ions. While the distribution of accelerated particles integrated over the whole simulation box appears highly non-thermal, it is actually the superposition of a series of distributions in different sectors of a 2D magnetic island. Each of those distributions has only a small non-thermal component compared with its thermal core. By tracking a large number of particles, we show that particles get energized in X-line regions, contracting magnetic islands, and magnetic island coalescence regions. We obtain the particle energization rate ${\boldsymbol{j}}\cdot {\boldsymbol{E}}$ by averaging over particle drift motions and find that it agrees well with the particle kinetic energy change. We quantify the contribution of curvature drift, gradient drift, polarization drift, magnetization, non-gyrotropic effect, and parallel electric field in different acceleration regions. We find that the major energization is due to particle curvature drift along the motional electric field. The other particle motions contribute less but may become important in different acceleration regions. The highly efficient particle energization in low-β plasmas may help us understand the strong particle energization in solar flares and accretion disk coronae.},
doi = {10.3847/1538-4357/aa745e},
journal = {The Astrophysical Journal (Online)},
number = 1,
volume = 843,
place = {United States},
year = {Tue Jun 27 00:00:00 EDT 2017},
month = {Tue Jun 27 00:00:00 EDT 2017}
}

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Cited by: 77 works
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Figures / Tables:

Figure 1 Figure 1: (a) Out-of-plane magnetic field $B$y in run R1 at $tΩ$$ci$ = 60, 152.5, and 800. The arrow in the middle panel indicates one representative island-merging region. (b) The bulk flow velocity in run R1 at $tΩ$$ci$ = 60 and 152.5. The dashed lines in the upper two panelsmore » are a horizontal cut along $z$=0. Plotted in the bottom panel is $v$$x$ along the cut. The red line is the cut at $tΩ$$ci$ =60 . The blue line is the cut at $tΩ$$ci$ = 152.5. $v$$x$ is normalized to the reconnection inflow Alfvén speed $v$$A$. The overplotted arrow indicates a reconnection $X$-point, indicated by the bi-directional reconnection outflow.« less

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