Your browser doesn't support javascript.
loading
Cerenkov emission of quasiparallel whistlers by fast electron phase-space holes during magnetic reconnection.
Goldman, M V; Newman, D L; Lapenta, G; Andersson, L; Gosling, J T; Eriksson, S; Markidis, S; Eastwood, J P; Ergun, R.
Afiliação
  • Goldman MV; University of Colorado, Boulder, Colorado 80309, USA.
  • Newman DL; University of Colorado, Boulder, Colorado 80309, USA.
  • Lapenta G; Leuven Universiteit, Celestijnenlaan 200B, B-2001 Leuven, Belgium.
  • Andersson L; University of Colorado, Boulder, Colorado 80309, USA.
  • Gosling JT; University of Colorado, Boulder, Colorado 80309, USA.
  • Eriksson S; University of Colorado, Boulder, Colorado 80309, USA.
  • Markidis S; KTH Royal Institute of Technology, SE-100 44 Stockholm, Sweden.
  • Eastwood JP; The Blackett Laboratory, Imperial College London, SW7 2AZ London, United Kingdom.
  • Ergun R; University of Colorado, Boulder, Colorado 80309, USA.
Phys Rev Lett ; 112(14): 145002, 2014 Apr 11.
Article em En | MEDLINE | ID: mdl-24765977
ABSTRACT
Kinetic simulations of magnetotail reconnection have revealed electromagnetic whistlers originating near the exhaust boundary and propagating into the inflow region. The whistler production mechanism is not a linear instability, but rather is Cerenkov emission of almost parallel whistlers from localized moving clumps of charge (finite-size quasiparticles) associated with nonlinear coherent electron phase space holes. Whistlers are strongly excited by holes without ever growing exponentially. In the simulation the whistlers are emitted in the source region from holes that accelerate down the magnetic separatrix towards the x line. The phase velocity of the whistlers vφ in the source region is everywhere well matched to the hole velocity vH as required by the Cerenkov condition. The simulation shows emission is most efficient near the theoretical maximum vφ=half the electron Alfven speed, consistent with the new theoretical prediction that faster holes radiate more efficiently. While transferring energy to whistlers the holes lose coherence and dissipate over a few local ion inertial lengths. The whistlers, however, propagate to the x line and out over many 10's of ion inertial lengths into the inflow region of reconnection. As the whistlers pass near the x line they modulate the rate at which magnetic field lines reconnect.
Buscar no Google
Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2014 Tipo de documento: Article
Buscar no Google
Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2014 Tipo de documento: Article