Global hybrid (electron fluid, kinetic ions) and fully kinetic simulations of the magnetosphere have been used to show surprising interconnection between shocks, turbulence, and magnetic reconnection. In particular, collisionless shocks with their reflected ions that can get upstream before retransmission can generate previously unforeseen phenomena in the post shocked flows: (i) formation of reconnecting current sheets and magnetic islands with sizes up to tens of ion inertial length. (ii) Generation of large scale low frequency electromagnetic waves that are compressed and amplified as they cross the shock. These “wavefronts” maintain their integrity for tens of ion cyclotron times but eventually disrupt and dissipate their energy. (iii) Rippling of the shock front, which can in turn lead to formation of fast collimated jets extending to hundreds of ion inertial lengths downstream of the shock. The jets, which have high dynamical pressure, “stir” the downstream region, creating large scale disturbances such as vortices, sunward flows, and can trigger flux ropes along the magnetopause. This phenomenology closes the loop between shocks, turbulence, and magnetic reconnection in ways previously unrealized. These interconnections appear generic for the collisionless plasmas typical of space and are expected even at planar shocks, although they will also occur at curved shocks as occur at planets or around ejecta.
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June 2014
Research Article|
June 18 2014
The link between shocks, turbulence, and magnetic reconnection in collisionless plasmas
H. Karimabadi;
H. Karimabadi
1
University of California
, San Diego, La Jolla, California 92093, USA
2SciberQuest, Inc., Del Mar, California 92014,
USA
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V. Roytershteyn;
V. Roytershteyn
2SciberQuest, Inc., Del Mar, California 92014,
USA
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H. X. Vu;
H. X. Vu
2SciberQuest, Inc., Del Mar, California 92014,
USA
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Y. A. Omelchenko;
Y. A. Omelchenko
1
University of California
, San Diego, La Jolla, California 92093, USA
2SciberQuest, Inc., Del Mar, California 92014,
USA
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J. Scudder;
J. Scudder
3
University of Iowa
, Iowa City, Iowa 52242, USA
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W. Daughton;
W. Daughton
4
Los Alamos National Laboratory
, Los Alamos, New Mexico 87545, USA
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A. Dimmock;
A. Dimmock
5
Aalto University
, Espoo, Finland
6
Embry Riddle Aeronautical University
, Florida 32114, USA
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K. Nykyri;
K. Nykyri
5
Aalto University
, Espoo, Finland
6
Embry Riddle Aeronautical University
, Florida 32114, USA
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M. Wan;
M. Wan
7
University of Delaware
, Newark, Delaware 19716, USA
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D. Sibeck;
D. Sibeck
8
NASA Goddard Space Flight Center
, Greenbelt, Maryland 20771, USA
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M. Tatineni;
M. Tatineni
9
San Diego Supercomputer Center
, La Jolla, California 92093, USA
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A. Majumdar;
A. Majumdar
9
San Diego Supercomputer Center
, La Jolla, California 92093, USA
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B. Loring;
B. Loring
10
Lawrence Berkeley National Laboratory
, Berkeley, California 94720, USA
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B. Geveci
B. Geveci
11Kitware, New York 12065,
USA
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Phys. Plasmas 21, 062308 (2014)
Article history
Received:
February 26 2014
Accepted:
May 07 2014
Citation
H. Karimabadi, V. Roytershteyn, H. X. Vu, Y. A. Omelchenko, J. Scudder, W. Daughton, A. Dimmock, K. Nykyri, M. Wan, D. Sibeck, M. Tatineni, A. Majumdar, B. Loring, B. Geveci; The link between shocks, turbulence, and magnetic reconnection in collisionless plasmas. Phys. Plasmas 1 June 2014; 21 (6): 062308. https://doi.org/10.1063/1.4882875
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