Transport hysteresis in electromagnetic microturbulence caused by mesoscale zonal flow pattern-induced mitigation of high β turbulence runaways

Electromagnetic microturbulence at finite normalized plasma pressure β = n 0 T 0 / (B 0 2 / 2 μ 0) (n0 is the equilibrium density, T0 the equilibrium temperature, B0 the equilibrium magnetic field, and μ0 the permeability of free space) is investigated within a local gradient-driven gyrokinetic fram...

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Bibliographic Details
Main Authors: Peeters, A.G (Author), Rath, F. (Author)
Format: Article
Language:English
Published: American Institute of Physics Inc. 2022
Subjects:
Online Access:View Fulltext in Publisher
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020 |a 1070664X (ISSN) 
245 1 0 |a Transport hysteresis in electromagnetic microturbulence caused by mesoscale zonal flow pattern-induced mitigation of high β turbulence runaways 
260 0 |b American Institute of Physics Inc.  |c 2022 
856 |z View Fulltext in Publisher  |u https://doi.org/10.1063/5.0081846 
520 3 |a Electromagnetic microturbulence at finite normalized plasma pressure β = n 0 T 0 / (B 0 2 / 2 μ 0) (n0 is the equilibrium density, T0 the equilibrium temperature, B0 the equilibrium magnetic field, and μ0 the permeability of free space) is investigated within a local gradient-driven gyrokinetic framework. The focus lies on the well-known high β turbulence runaways [R. E. Waltz, Phys. Plasmas 17, 072501 (2010)] that have been proposed to set a nonlinear upper threshold β c, also known as the nonzonal transition [M. J. Pueschel, Phys. Rev. Lett. 110, 155005 (2013)]. In this paper, it is shown that persistent mesoscale zonal flow patterns, developing self-consistently on long time scales, mitigate high β turbulence runaways. The application of such mesoscale zonal flow states as initial conditions allows for the access of an improved β-regime, that is, β > β c, in which no turbulence runaway occurs. Various aspects of those mesoscale zonal flow-dominated improved states are investigated, such as (i) the stability constraints with respect to the mesoscale zonal flow level for the triggering of turbulence runaways, (ii) the influence of mesoscale zonal flows on magnetic stochasticity [W. M. Nevins, Phys. Rev. Lett. 106, 065003 (2010)], and (iii) the transfer processes connected to the drive and damping of mesoscale zonal flows. This work implies that β c does not set the upper limit in the normalized plasma pressure for stationary operation, provided persistent mesoscale zonal flow patterns can develop. Since variations of β occur on the energy confinement time, which is large compared to the time required for mesoscale zonal flows to develop, the reported mesoscale zonal flow-dominated improved β-regime is expected to be the experimentally relevant branch. Furthermore, this work highlights the need for sufficiently long simulation time traces of at least a few ∼ 10 3 R 0 / v th, i (R0 is the major radius, and v th, i is the ion thermal velocity), also within kinetic electron frameworks, to capture non-negligible long-term dynamics. © 2022 Author(s). 
650 0 4 |a Electromagnetics 
650 0 4 |a Equilibrium density 
650 0 4 |a Equilibrium temperatures 
650 0 4 |a Flow patterns 
650 0 4 |a Free spaces 
650 0 4 |a Gradient-driven 
650 0 4 |a Hysteresis 
650 0 4 |a Local gradients 
650 0 4 |a Magnetic-field 
650 0 4 |a Mesoscale zonal flows 
650 0 4 |a Microturbulence 
650 0 4 |a Plasma pressures 
650 0 4 |a Plasma stability 
650 0 4 |a Turbulence 
700 1 |a Peeters, A.G.  |e author 
700 1 |a Rath, F.  |e author 
773 |t Physics of Plasmas