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In the vicinity of X-line, even electrons become demagnetized and diffuse, thus we call this region electron diffusion region.
In strongly asymmetric reconnection layers with negligible guide field, the energy deposition to electrons is found to primarily occur in the electron diffusion region where electrons are demagnetized and diffuse.
In the reconnection layers without guide field, it was found that the energy deposition to electrons primarily occurs through je⊥·E⊥ (where E⊥is the electric field perpendicular to the magnetic field and je is the electron current density) and is concentrated in the electron diffusion region where electrons are demagnetized and diffuse.
Figure 3 presents energy conversion to electrons in the electron diffusion region during magnetopause reconnection.
Burlingame, Q. et al. Centimetre-scale electron diffusion in photoactive organic heterostructures.
Figure 3a shows the approximate MMS trajectory through the electron diffusion region on the profile of JY.
Torbert, R. B. et al. Estimates of terms in Ohm's law during an encounter with an electron diffusion region.
A longer electron diffusion length is favourable for enhancing efficiency.
It has been considered that the electron pressure tensor term and/or fluctuations can generate energy dissipation particularly at the electron diffusion region2,27,28,29.
One of the most important results of MRX-MMS collaboration has been to clarify the role of the electron diffusion region together with the energy deposition to electrons.
Energy deposition to electrons peaks at the electron diffusion region through the work done by the reconnection electric field as demonstrated in Fig. 3.
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