Electromagnetic total-f algorithm for gyrokinetic particle-in-cell simulations of boundary plasma in XGC

Hager, Robert; Ku, Seung-Hoe; Sharma, Amil Y.; Churchill, Randy Michael; Chang, C. S.; Scheinberg, Aaron
Issue date: 21 November 2022
Cite as:
Hager, Robert, Ku, Seung-Hoe, Sharma, Amil Y., Churchill, Randy Michael, Chang, C. S., & Scheinberg, Aaron. (2023). Electromagnetic total-f algorithm for gyrokinetic particle-in-cell simulations of boundary plasma in XGC [Data set]. Princeton Plasma Physics Laboratory, Theory Department.
@electronic{hager_robert_2023,
  author      = {Hager, Robert and
                Ku, Seung-Hoe and
                Sharma, Amil Y. and
                Churchill, Randy Michael and
                Chang, C. S. and
                Scheinberg, Aaron},
  title       = {{Electromagnetic total-f algorithm for gy
                rokinetic particle-in-cell simulations o
                f boundary plasma in XGC}},
  publisher   = {{Princeton Plasma Physics Laboratory, The
                ory Department}},
  year        = 2023
}
Abstract:

The simplified delta-f mixed-variable/pull-back electromagnetic simulation algorithm implemented in XGC for core plasma simulations by Cole et al. [Phys. Plasmas 28, 034501 (2021)] has been generalized to a total-f electromagnetic algorithm that can include, for the first time, the boundary plasma in diverted magnetic geometry with neutral particle recycling, turbulence and neoclassical physics. The delta-f mixed-variable/pull-back electromagnetic implementation is based on the pioneering work by Kleiber and Mischenko et al. [Kleiber et al., Phys. Plasmas 23, 032501 (2016); Mishchenko et al., Comput. Phys. Commun. 238, 194 (2019)]. An electromagnetic demonstration simulation is performed in a DIII-D-like, H-mode boundary plasma, including a corresponding comparative electrostatic simulation, which confirms that the electromagnetic simulation is necessary for a higher fidelity understanding of the electron particle and heat transport even at the low-beta pedestal foot in the vicinity of the magnetic separatrix.

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