2015
DOI: 10.1002/2014ja020795
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Structure of exhaust jets produced by magnetic reconnection localized in the out‐of‐plane direction

Abstract: Three‐dimensional electromagnetic particle‐in‐cell simulations are used to investigate the structure of exhaust jets produced by magnetic reconnection localized in the out‐of‐plane direction. The localized reconnection is produced by periodically blocking the cross‐tail current density, a procedure that has effects analogous to those produced by the assumption of a region of anomalous resistivity in fluid treatments of reconnection. The width of the blocking region is varied between 4 and 24di, where di is the… Show more

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Cited by 20 publications
(45 citation statements)
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“…Also, a clear smaller-scale (∼1-2d i ) structure has appeared within both segments, and there is also a faint precursor modulation in B z on a similar scale visible ahead of the front. As discussed in Pritchett (2015), this smaller scale structure is consistent with the growth of the ballooning/interchange instability (BICI), but it is larger than the scale expected for the lower hybrid drift instability that peaks at wavelengths satisfying k y ρ e ≈ 1 (e.g., Daughton 2003), which corresponds to a length of 0.3d i . Figure 1b shows the B z structure of the front at the later time i0 t = 53.…”
Section: Overview Of Jet Expansionsupporting
confidence: 69%
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“…Also, a clear smaller-scale (∼1-2d i ) structure has appeared within both segments, and there is also a faint precursor modulation in B z on a similar scale visible ahead of the front. As discussed in Pritchett (2015), this smaller scale structure is consistent with the growth of the ballooning/interchange instability (BICI), but it is larger than the scale expected for the lower hybrid drift instability that peaks at wavelengths satisfying k y ρ e ≈ 1 (e.g., Daughton 2003), which corresponds to a length of 0.3d i . Figure 1b shows the B z structure of the front at the later time i0 t = 53.…”
Section: Overview Of Jet Expansionsupporting
confidence: 69%
“…1a, b. Thus the ion flow is being decelerated at the front itself (Drake et al 2014;Pritchett 2015). This increase in flow speed behind the main DF is also observed in the THEMIS P1 event, with a peak speed of nearly 1000 km/s observed 45 s after the main DF.…”
Section: Overview Of Jet Expansionmentioning
confidence: 60%
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