Electromagnetic zonal flow residual responses

Journal of Plasma Physics Cambridge University Press 83:4 (2017) 1-38

Authors:

PJ Catto, FI Parra, I Pusztai

Abstract:

The collisionless axisymmetric zonal flow residual calculation for a tokamak plasma is generalized to include electromagnetic perturbations. We formulate and solve the complete initial value zonal flow problem by retaining the fully self-consistent axisymmetric spatial perturbations in the electric and magnetic fields. Simple expressions for the electrostatic, shear and compressional magnetic residual responses are derived that provide a fully electromagnetic test of the zonal flow residual in gyrokinetic codes. Unlike the electrostatic potential, the parallel vector potential and the parallel magnetic field perturbations need not relax to flux functions for all possible initial conditions.

Distribution functions for resonantly trapped orbits in the Galactic disc

Monthly Notices of the Royal Astronomical Society Oxford University Press 471:4 (2017) 4314-4322

Authors:

G Monari, B Famaey, J-B Fouvry, James Binney

Abstract:

The present-day response of a Galactic disc stellar population to a non-axisymmetric perturbation of the potential has previously been computed through perturbation theory within the phase-space coordinates of the unperturbed axisymmetric system. Such an Eulerian linearized treatment, however, leads to singularities at resonances, which prevent quantitative comparisons with data. Here, we manage to capture the behaviour of the distribution function (DF) at a resonance in a Lagrangian approach, by averaging the Hamiltonian over fast angle variables and re-expressing the DF in terms of a new set of canonical actions and angles variables valid in the resonant region. We then follow the prescription of Binney, assigning to the resonant DF the time average along the orbits of the axisymmetric DF expressed in the new set of actions and angles. This boils down to phase-mixing the DF in terms of the new angles, such that the DF for trapped orbits depends only on the new set of actions. This opens the way to quantitatively fitting the effects of the bar and spirals to Gaia data in terms of DFs in action space.

Distribution functions for Galactic disc stellar populations in the presence of non-axisymmetric perturbations

Proceedings of the International Astronomical Union Cambridge University Press (CUP) 13:S334 (2017) 195-198

Authors:

B Famaey, G Monari, A Siebert, J-B Fouvry, J Binney

Black Hole Mergers in Galactic Nuclei Induced by the Eccentric Kozai-Lidov Effect

(2017)

Authors:

Bao-Minh Hoang, Smadar Naoz, Bence Kocsis, Frederic A Rasio, Fani Dosopoulou

Overview of recent physics results from MAST

Nuclear Fusion Institute of Physics 57:10 (2017) 102007

Authors:

A Kirk, J Adamek, RJ Akers, S Allan, L Appel, F Arese Lucini, Michael Barnes, T Barrett, N Ben Ayed, W Boeglin, J Bradley, PK Browning, J Brunner, P Cahyna, S Cardnell, M Carr, F Casson, M Cecconello, C Challis, IT Chapman, S Chapman, J Chorley, S Conroy, N Conway, WA Cooper

Abstract:

New results from MAST are presented that focus on validating models in order to extrapolate to future devices. Measurements during start-up experiments have shown how the bulk ion temperature rise scales with the square of the reconnecting field. During the current ramp-up, models are not able to correctly predict the current diffusion. Experiments have been performed looking at edge and core turbulence. At the edge, detailed studies have revealed how filament characteristics are responsible for determining the near and far scrape off layer density profiles. In the core the intrinsic rotation and electron scale turbulence have been measured. The role that the fast ion gradient has on redistributing fast ions through fishbone modes has led to a redesign of the neutral beam injector on MAST Upgrade. In H-mode the turbulence at the pedestal top has been shown to be consistent with being due to electron temperature gradient modes. A reconnection process appears to occur during edge localized modes (ELMs) and the number of filaments released determines the power profile at the divertor. Resonant magnetic perturbations can mitigate ELMs provided the edge peeling response is maximised and the core kink response minimised. The mitigation of intrinsic error fields with toroidal mode number n > 1 has been shown to be important for plasma performance.