Density cavity in magnetic reconnection diffusion region in the presence of guide field
Density cavity in magnetic reconnection diffusion region in the presence of guide field
复制标题
存在导场时磁重联扩散区的密度空腔
DOI:
10.1029/2010ja016324
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发表时间:
2011-06
影响因子:
--
通讯作者:
Huang, S. Y.
中科院分区:
文献类型:
--
作者:
Zhou, M.;Pang, Y.;Deng, X. H.;Yuan, Z. G.;Huang, S. Y.
[1] Understanding the structure of the diffusion region of magnetic reconnection is crucial to pinpoint the mechanism of energy conversion from magnetic field to plasma. Characteristics of a diffusion region with guide field (i.e., component reconnection) may be significantly different from those of a diffusion region without guide field (i.e., antiparallel reconnection). In this study, we attempt to understand the structure of a diffusion region with guide field by studying the density cavity along separatrix. We present an event in which a density cavity was detected by the Cluster spacecraft in a diffusion region in the presence of guide field. The cavity was located around the separatrix region on the southern hemisphere of the neutral sheet and earthward of the X-line and was coincident with strong magnetic field compression. The width of the cavity was on the ion inertial scale. This cavity contained a relatively strong antiparallel current, which was mainly contributed by parallel streaming electrons with energy of 1–10 keV. Enhancements of lower hybrid wave and electromagnetic whistler wave were observed inside the cavity. These waves are probably excited by parallel streaming electrons along separatrix via electron beam instability. Two-dimensional electromagnetic particle-in-cell simulation was employed to study the structure of the density cavity. The location and scale of the cavity and the signature of electric current and electron velocity are consistent with our observations. It is found that there was displacement between the position of electron density minimum and out-of-plane magnetic field maximum in reconnection with guide field. However, this displacement is much less than that in reconnection without guide field. There was no significant acceleration for electrons to reach energy larger than 30 keV at the cavity.
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影响因子:
10.3
作者:
Georg Gustafsson;R. Boström;B. Holback;G. Holmgren;A. Lundgren;Krzysztof Stasiewicz;L. Åhlén;
通讯作者:
Georg Gustafsson;R. Boström;B. Holback;G. Holmgren;A. Lundgren;Krzysztof Stasiewicz;L. Åhlén;
影响因子:
2.2
作者:
Daughton, William;Scudder, Jack;Karimabadi, Homa
通讯作者:
Karimabadi, Homa
影响因子:
--
作者:
Shiyong Huang;Meng Zhou;F. Sahraoui;X. Deng;Y. Pang;Z. Yuan;Q. Wei;J. Wang;Xueying Zhou
通讯作者:
Shiyong Huang;Meng Zhou;F. Sahraoui;X. Deng;Y. Pang;Z. Yuan;Q. Wei;J. Wang;Xueying Zhou
影响因子:
--
作者:
T. Nagai;I. Shinohara;M. Fujimoto;S. Machida;R. Nakamura;Y. Saito;T. Mukai
通讯作者:
T. Nagai;I. Shinohara;M. Fujimoto;S. Machida;R. Nakamura;Y. Saito;T. Mukai
影响因子:
8.6
作者:
A. Teste;G. Parks
通讯作者:
A. Teste;G. Parks