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- W4353032098 abstract "Abstract We implement the higher order gyrokinetic theory developed in Dudkovskaia et al (2023 Plasma Phys. Control. Fusion 65 045010), reduced to the limit of <?CDATA $B_{vartheta} / B_0 ll 1$?> <mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML overflow=scroll> <mml:msub> <mml:mi>B</mml:mi> <mml:mrow> <mml:mi>ϑ</mml:mi> </mml:mrow> </mml:msub> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:msub> <mml:mi>B</mml:mi> <mml:mn>0</mml:mn> </mml:msub> <mml:mo>≪</mml:mo> <mml:mn>1</mml:mn> </mml:math> , where B 0 is the tokamak equilibrium magnetic field, and B ϑ is its poloidal component, in the local gyrokinetic turbulence code, GS2. The principal motivation for this extension is to quantify the importance of neoclassical flows in electromagnetic gyrokinetics, with a particular interest in sharp pressure gradient regions where the bootstrap current becomes dominant. To incorporate neoclassical equilibrium physics, GS2 is coupled to NEO, a multi-species drift kinetic solver. It is found that the regions where microinstabilities are most likely to be influenced by neoclassical equilibrium effects are in a pedestal plasma and a spherical tokamak core plasma." @default.
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- W4353032098 date "2023-04-12" @default.
- W4353032098 modified "2023-09-27" @default.
- W4353032098 title "Quantifying the role of higher order neoclassical corrections to gyrokinetics in tokamak plasmas" @default.
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- W4353032098 doi "https://doi.org/10.1088/1361-6587/acc688" @default.
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