2007
DOI: 10.1134/s1063780x07060013
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Magnetic structure of current sheets in magnetic fields with a singular X line

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Cited by 22 publications
(2 citation statements)
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“…The current J Z initiated 2D plasma flows in the magnetic field → B, and gave rise to the current sheet formation during the first 1-1.5 µs. The typical transverse sizes of the current sheet were: 2δx ≈ 12-17 cm (width) and 2δy ≈ 1.5-3.5 cm (thickness), at the level of 0.1 • j 0 z ; here, j 0 z is the current density at the middle plane of the sheet [27,28]. The sheet length along the direction of the current was equal to ∆z.…”
Section: Experimental Setup and Methods Of Diagnosticsmentioning
confidence: 99%
“…The current J Z initiated 2D plasma flows in the magnetic field → B, and gave rise to the current sheet formation during the first 1-1.5 µs. The typical transverse sizes of the current sheet were: 2δx ≈ 12-17 cm (width) and 2δy ≈ 1.5-3.5 cm (thickness), at the level of 0.1 • j 0 z ; here, j 0 z is the current density at the middle plane of the sheet [27,28]. The sheet length along the direction of the current was equal to ∆z.…”
Section: Experimental Setup and Methods Of Diagnosticsmentioning
confidence: 99%
“…4 In geospace, global effects of reconnection are generally associated with X-points along separators (Dorelli et al 2007a,b), however, in the solar corona large amounts of stored energy appear to be released at magnetic nulls (see e.g., Antiochos et al 2002). Several regimes of non-ideal behavior and reconnection at magnetic null points have been hypothesized and modeled theoretically (Priest and Titov 1996;Pontin et al 2005;Parnell 2007;Priest and Pontin 2009;Wyper and Jain 2010;Galsgaard and Pontin 2011a,b;Pontin et al 2011), studied in the laboratory (Bogdanov et al 1994;Lukin and Linton 2011), and inferred from coronal observations (Parnell 2007;Parnell et al 2008).…”
Section: Plasma Phenomena As Measured In Three Dimensionsmentioning
confidence: 99%