2012
DOI: 10.1016/j.cnsns.2011.04.029
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Quasi-separatrix layers and three-dimensional reconnection diagnostics for line-tied tearing modes

Abstract: In three-dimensional magnetic configurations for a plasma in which no closed field line or magnetic null exists, no magnetic reconnection can occur, by the strictest definition of reconnection. A finitely long pinch with line-tied boundary conditions, in which all the magnetic field lines start at one end of the system and proceed to the opposite end, is an example of such a system. Nevertheless, for a long system of this type, the physical behavior in resistive magnetohydrodynamics (MHD) essentially involves … Show more

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Cited by 12 publications
(22 citation statements)
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“…These works highlight the key role of magnetic separator surfaces, surfaces across which the field line connectivity changes discontinuously. The role of separator surfaces as likely sites for current sheet formation and reconnection has been further generalized to systems that lack null points through the introduction of quasi-separatrix layers (QSLs) [44][45][46]. QSLs have been identified in the LAPD experiment and in kinetic simulations of line-tied reconnection [47].…”
Section: (B) Reconnection In Line-tied Magnetic Fieldsmentioning
confidence: 99%
“…These works highlight the key role of magnetic separator surfaces, surfaces across which the field line connectivity changes discontinuously. The role of separator surfaces as likely sites for current sheet formation and reconnection has been further generalized to systems that lack null points through the introduction of quasi-separatrix layers (QSLs) [44][45][46]. QSLs have been identified in the LAPD experiment and in kinetic simulations of line-tied reconnection [47].…”
Section: (B) Reconnection In Line-tied Magnetic Fieldsmentioning
confidence: 99%
“…The computation of this indicator is of similar complexity to the identification of null points but detects also other types of more complex 3D reconnnection topologies. The new indicator is simpler compared to other methods to find these complex 3D magnetic reconnection topologies such as the squashing factor (Titov et al 2002;Finn et al 2014) and the field integrated parallel potential (Lau & Finn 1990;Richardson & Finn 2012) that requires complex integration along the field lines and even of the agyrotropy (Scudder & Daughton 2008) that requires one to compute the eigenvalues of the pressure tensor. The proposed indicator is a local operation that requires only the knowledge of the local magnetic and electric field: it can be applied in a simulation or in observational data from a field instrument.…”
Section: Introductionmentioning
confidence: 99%
“…QSLs are the locations where these non-idealnesses can occur; therefore, the two approaches are complementary (Démoulin et al 1996b;Richardson & Finn 2012).…”
Section: Introductionmentioning
confidence: 99%