author_facet Hietala, H.
Drake, J. F.
Phan, T. D.
Eastwood, J. P.
McFadden, J. P.
Hietala, H.
Drake, J. F.
Phan, T. D.
Eastwood, J. P.
McFadden, J. P.
author Hietala, H.
Drake, J. F.
Phan, T. D.
Eastwood, J. P.
McFadden, J. P.
spellingShingle Hietala, H.
Drake, J. F.
Phan, T. D.
Eastwood, J. P.
McFadden, J. P.
Geophysical Research Letters
Ion temperature anisotropy across a magnetotail reconnection jet
General Earth and Planetary Sciences
Geophysics
author_sort hietala, h.
spelling Hietala, H. Drake, J. F. Phan, T. D. Eastwood, J. P. McFadden, J. P. 0094-8276 1944-8007 American Geophysical Union (AGU) General Earth and Planetary Sciences Geophysics http://dx.doi.org/10.1002/2015gl065168 <jats:title>Abstract</jats:title><jats:p>A significant fraction of the energy released by magnetotail reconnection appears to go into ion heating, but this heating is generally anisotropic. We examine ARTEMIS dual‐spacecraft observations of a long‐duration magnetotail exhaust generated by antiparallel reconnection in conjunction with particle‐in‐cell simulations, showing spatial variations in the anisotropy across the outflow far (&gt;100<jats:italic>d</jats:italic><jats:sub><jats:italic>i</jats:italic></jats:sub>) downstream of the X line. A consistent pattern is found in both the spacecraft data and the simulations: While the total temperature across the exhaust is rather constant, near the boundaries <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> dominates. The plasma is well above the firehose threshold within patchy spatial regions at |<jats:italic>B</jats:italic><jats:sub><jats:italic>X</jats:italic></jats:sub>|∈[0.1,0.5]<jats:italic>B</jats:italic><jats:sub>0</jats:sub>, suggesting that the drive for the instability is strong and the instability is too weak to relax the anisotropy. At the midplane ( <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/grl53378-math-0001.png" xlink:title="urn:x-wiley:grl:media:grl53378:grl53378-math-0001" />), <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,⊥</jats:sub>&gt;<jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> and ions undergo Speiser‐like motion despite the large distance from the X line.</jats:p> Ion temperature anisotropy across a magnetotail reconnection jet Geophysical Research Letters
doi_str_mv 10.1002/2015gl065168
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series Geophysical Research Letters
source_id 49
title Ion temperature anisotropy across a magnetotail reconnection jet
title_unstemmed Ion temperature anisotropy across a magnetotail reconnection jet
title_full Ion temperature anisotropy across a magnetotail reconnection jet
title_fullStr Ion temperature anisotropy across a magnetotail reconnection jet
title_full_unstemmed Ion temperature anisotropy across a magnetotail reconnection jet
title_short Ion temperature anisotropy across a magnetotail reconnection jet
title_sort ion temperature anisotropy across a magnetotail reconnection jet
topic General Earth and Planetary Sciences
Geophysics
url http://dx.doi.org/10.1002/2015gl065168
publishDate 2015
physical 7239-7247
description <jats:title>Abstract</jats:title><jats:p>A significant fraction of the energy released by magnetotail reconnection appears to go into ion heating, but this heating is generally anisotropic. We examine ARTEMIS dual‐spacecraft observations of a long‐duration magnetotail exhaust generated by antiparallel reconnection in conjunction with particle‐in‐cell simulations, showing spatial variations in the anisotropy across the outflow far (&gt;100<jats:italic>d</jats:italic><jats:sub><jats:italic>i</jats:italic></jats:sub>) downstream of the X line. A consistent pattern is found in both the spacecraft data and the simulations: While the total temperature across the exhaust is rather constant, near the boundaries <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> dominates. The plasma is well above the firehose threshold within patchy spatial regions at |<jats:italic>B</jats:italic><jats:sub><jats:italic>X</jats:italic></jats:sub>|∈[0.1,0.5]<jats:italic>B</jats:italic><jats:sub>0</jats:sub>, suggesting that the drive for the instability is strong and the instability is too weak to relax the anisotropy. At the midplane ( <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/grl53378-math-0001.png" xlink:title="urn:x-wiley:grl:media:grl53378:grl53378-math-0001" />), <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,⊥</jats:sub>&gt;<jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> and ions undergo Speiser‐like motion despite the large distance from the X line.</jats:p>
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author Hietala, H., Drake, J. F., Phan, T. D., Eastwood, J. P., McFadden, J. P.
author_facet Hietala, H., Drake, J. F., Phan, T. D., Eastwood, J. P., McFadden, J. P., Hietala, H., Drake, J. F., Phan, T. D., Eastwood, J. P., McFadden, J. P.
author_sort hietala, h.
container_issue 18
container_start_page 7239
container_title Geophysical Research Letters
container_volume 42
description <jats:title>Abstract</jats:title><jats:p>A significant fraction of the energy released by magnetotail reconnection appears to go into ion heating, but this heating is generally anisotropic. We examine ARTEMIS dual‐spacecraft observations of a long‐duration magnetotail exhaust generated by antiparallel reconnection in conjunction with particle‐in‐cell simulations, showing spatial variations in the anisotropy across the outflow far (&gt;100<jats:italic>d</jats:italic><jats:sub><jats:italic>i</jats:italic></jats:sub>) downstream of the X line. A consistent pattern is found in both the spacecraft data and the simulations: While the total temperature across the exhaust is rather constant, near the boundaries <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> dominates. The plasma is well above the firehose threshold within patchy spatial regions at |<jats:italic>B</jats:italic><jats:sub><jats:italic>X</jats:italic></jats:sub>|∈[0.1,0.5]<jats:italic>B</jats:italic><jats:sub>0</jats:sub>, suggesting that the drive for the instability is strong and the instability is too weak to relax the anisotropy. At the midplane ( <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/grl53378-math-0001.png" xlink:title="urn:x-wiley:grl:media:grl53378:grl53378-math-0001" />), <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,⊥</jats:sub>&gt;<jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> and ions undergo Speiser‐like motion despite the large distance from the X line.</jats:p>
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imprint_str_mv American Geophysical Union (AGU), 2015
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spelling Hietala, H. Drake, J. F. Phan, T. D. Eastwood, J. P. McFadden, J. P. 0094-8276 1944-8007 American Geophysical Union (AGU) General Earth and Planetary Sciences Geophysics http://dx.doi.org/10.1002/2015gl065168 <jats:title>Abstract</jats:title><jats:p>A significant fraction of the energy released by magnetotail reconnection appears to go into ion heating, but this heating is generally anisotropic. We examine ARTEMIS dual‐spacecraft observations of a long‐duration magnetotail exhaust generated by antiparallel reconnection in conjunction with particle‐in‐cell simulations, showing spatial variations in the anisotropy across the outflow far (&gt;100<jats:italic>d</jats:italic><jats:sub><jats:italic>i</jats:italic></jats:sub>) downstream of the X line. A consistent pattern is found in both the spacecraft data and the simulations: While the total temperature across the exhaust is rather constant, near the boundaries <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> dominates. The plasma is well above the firehose threshold within patchy spatial regions at |<jats:italic>B</jats:italic><jats:sub><jats:italic>X</jats:italic></jats:sub>|∈[0.1,0.5]<jats:italic>B</jats:italic><jats:sub>0</jats:sub>, suggesting that the drive for the instability is strong and the instability is too weak to relax the anisotropy. At the midplane ( <jats:inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="graphic/grl53378-math-0001.png" xlink:title="urn:x-wiley:grl:media:grl53378:grl53378-math-0001" />), <jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,⊥</jats:sub>&gt;<jats:italic>T</jats:italic><jats:sub><jats:italic>i</jats:italic>,||</jats:sub> and ions undergo Speiser‐like motion despite the large distance from the X line.</jats:p> Ion temperature anisotropy across a magnetotail reconnection jet Geophysical Research Letters
spellingShingle Hietala, H., Drake, J. F., Phan, T. D., Eastwood, J. P., McFadden, J. P., Geophysical Research Letters, Ion temperature anisotropy across a magnetotail reconnection jet, General Earth and Planetary Sciences, Geophysics
title Ion temperature anisotropy across a magnetotail reconnection jet
title_full Ion temperature anisotropy across a magnetotail reconnection jet
title_fullStr Ion temperature anisotropy across a magnetotail reconnection jet
title_full_unstemmed Ion temperature anisotropy across a magnetotail reconnection jet
title_short Ion temperature anisotropy across a magnetotail reconnection jet
title_sort ion temperature anisotropy across a magnetotail reconnection jet
title_unstemmed Ion temperature anisotropy across a magnetotail reconnection jet
topic General Earth and Planetary Sciences, Geophysics
url http://dx.doi.org/10.1002/2015gl065168