Energy partition between Alfvénic and compressive fluctuations in magnetorotational turbulence with near-azimuthal mean magnetic field

(2021)

Authors:

Y Kawazura, AA Schekochihin, M Barnes, W Dorland, SA Balbus

Inefficient magnetic-field amplification in supersonic laser-plasma turbulence

Physical Review Letters American Physical Society 127 (2021) 175002

Authors:

Afa Bott, L Chen, G Boutoux, T Caillaud, A Duval, M Koenig, B Khiar, I Lantuéjoul, L Le-Deroff, B Reville, R Rosch, D Ryu, C Spindloe, B Vauzour, B Villette, Aa Schekochihin, Dq Lamb, P Tzeferacos, G Gregori, A Casner

Abstract:

We report a laser-plasma experiment that was carried out at the LMJ-PETAL facility and realized the first magnetized, turbulent, supersonic plasma with a large magnetic Reynolds number ($\mathrm{Rm} \approx 45$) in the laboratory. Initial seed magnetic fields were amplified, but only moderately so, and did not become dynamically significant. A notable absence of magnetic energy at scales smaller than the outer scale of the turbulent cascade was also observed. Our results support the notion that moderately supersonic, low-magnetic-Prandtl-number plasma turbulence is inefficient at amplifying magnetic fields.

Gyrokinetic simulations in stellarators using different computational domains

Nuclear Fusion IOP Publishing 61:11 (2021) 116074

Authors:

E Sanchez, Jm Garcia-Regana, A Banon Navarro, Jhe Proll, C Mora Moreno, A Gonzalez-Jerez, I Calvo, R Kleiber, J Riemann, J Smoniewski, M Barnes, Fi Parra

Abstract:

In this work, we compare gyrokinetic simulations in stellarators using different computational domains, namely, flux tube (FT), full-flux-surface (FFS), and radially global (RG) domains. Two problems are studied: the linear relaxation of zonal flows (ZFs) and the linear stability of ion temperature gradient (ITG) modes. Simulations are carried out with the codes EUTERPE, GENE, GENE-3D, and stella in magnetic configurations of LHD and W7-X using adiabatic electrons. The ZF relaxation properties obtained in different FTs are found to differ with each other and with the RG result, except for sufficiently long FTs, in general. The FT length required for convergence is configuration-dependent. Similarly, for ITG instabilities, different FTs provide different results, but the discrepancy between them diminishes with increasing FT length. FFS and FT simulations show good agreement in the calculation of the growth rate and frequency of the most unstable modes in LHD, while for W7-X differences in the growth rates are found between the FT and the FFS domains. RG simulations provide results close to the FFS ones. The radial scale of unstable ITG modes is studied in global and FT simulations finding that in W7-X, the radial scale of the most unstable modes depends on the binormal wavenumber, while in LHD no clear dependency is found.

Astrophysical Gravitational-Wave Echoes from Galactic Nuclei

(2021)

Authors:

László Gondán, Bence Kocsis

DIII-D research advancing the physics basis for optimizing the tokamak approach to fusion energy

Nuclear Fusion IOP Publishing 62:4 (2021) 042024-042024

Authors:

ME Fenstermacher, for the DIII-D Team:, J Abbate, S Abe, T Abrams, M Adams, B Adamson, N Aiba, T Akiyama, P Aleynikov, E Allen, S Allen, H Anand, J Anderson, Y Andrew, T Andrews, D Appelt, R Arbon, N Ashikawa, A Ashourvan, M Aslin, Y Asnis, M Austin, D Ayala, J Bak

Abstract:

Publicación con muchos autores, entre ellos la investigadora de la Universidad de Sevilla: Cano Megías, PilarDIII-D physics research addresses critical challenges for the operation of ITER and the next generation of fusion energy devices. This is done through a focus on innovations to provide solutions for high performance long pulse operation, coupled with fundamental plasma physics understanding and model validation, to drive scenario development by integrating high performance core and boundary plasmas. Substantial increases in off-axis current drive efficiency from an innovative top launch system for EC power, and in pressure broadening for Alfven eigenmode control from a co-/counter-Ip steerable off-axis neutral beam, all improve the prospects for optimization of future long pulse/steady state high performance tokamak operation. Fundamental studies into the modes that drive the evolution of the pedestal pressure profile and electron vs ion heat flux validate predictive models of pedestal recovery after ELMs. Understanding the physics mechanisms of ELM control and density pumpout by 3D magnetic perturbation fields leads to confident predictions for ITER and future devices. Validated modeling of high-Z shattered pellet injection for disruption mitigation, runaway electron dissipation, and techniques for disruption prediction and avoidance including machine learning, give confidence in handling disruptivity for future devices. For the non-nuclear phase of ITER, two actuators are identified to lower the L–H threshold power in hydrogen plasmas. With this physics understanding and suite of capabilities, a high poloidal beta optimized-core scenario with an internal transport barrier that projects nearly to Q = 10 in ITER at ∼8 MA was coupled to a detached divertor, and a near super H-mode optimized-pedestal scenario with co-Ip beam injection was coupled to a radiative divertor. The hybrid core scenario was achieved directly, without the need for anomalous current diffusion, using off-axis current drive actuators. Also, a controller to assess proximity to stability limits and regulate βN in the ITER baseline scenario, based on plasma response to probing 3D fields, was demonstrated. Finally, innovative tokamak operation using a negative triangularity shape showed many attractive features for future pilot plant operation.US Department of Energy - Office of Science - Office of Fusion Energy Sciences DE-FC02- 04ER54698 y DE-AC52-07NA2734