Debye scale turbulence within the electron diffusion layer during magnetic reconnection

  • J. Jara-Almonte
    Center for Magnetic Self-Organization, Max-Planck/Princeton Center for Plasma Physics, Princeton Plasma Physics Laboratory 1 , Princeton, New Jersey 08543, USA
  • W. Daughton
    Los Alamos National Laboratory 2 , Los Alamos, New Mexico 87545, USA
  • H. Ji
    Center for Magnetic Self-Organization, Max-Planck/Princeton Center for Plasma Physics, Princeton Plasma Physics Laboratory 1 , Princeton, New Jersey 08543, USA

抄録

<jats:p>During collisionless, anti-parallel magnetic reconnection, the electron diffusion layer is the region of both fieldline breaking and plasma mixing. Due to the in-plane electrostatic fields associated with collisionless reconnection, the inflowing plasmas are accelerated towards the X-line and form counter-streaming beams within the unmagnetized diffusion layer. This configuration is inherently unstable to in-plane electrostatic streaming instabilities provided that there is sufficient scale separation between the Debye length λD and the electron skin depth c/ωpe. This scale separation has hitherto not been well resolved in kinetic simulations. Using both 2D fully kinetic simulations and a simple linear model, we demonstrate that these in-plane streaming instabilities generate Debye scale turbulence within the electron diffusion layer at electron temperatures relevant to magnetic reconnection both in the magnetosphere and in laboratory experiments.</jats:p>

収録刊行物

被引用文献 (1)*注記

もっと見る

キーワード

詳細情報 詳細情報について

問題の指摘

ページトップへ