Zero-turbulence manifold in a toroidal plasma.

Physical review letters 109:26 (2012) 265001

Authors:

EG Highcock, AA Schekochihin, SC Cowley, M Barnes, FI Parra, CM Roach, W Dorland

Abstract:

Sheared toroidal flows can cause bifurcations to zero-turbulent-transport states in tokamak plasmas. The maximum temperature gradients that can be reached are limited by subcritical turbulence driven by the parallel velocity gradient. Here it is shown that q/ϵ (magnetic field pitch/inverse aspect ratio) is a critical control parameter for sheared tokamak turbulence. By reducing q/ϵ, far higher temperature gradients can be achieved without triggering turbulence, in some instances comparable to those found experimentally in transport barriers. The zero-turbulence manifold is mapped out, in the zero-magnetic-shear limit, over the parameter space (γ(E), q/ϵ, R/L(T)), where γ(E) is the perpendicular flow shear and R/L(T) is the normalized inverse temperature gradient scale. The extent to which it can be constructed from linear theory is discussed.

High Frequency Gravitational Waves from Supermassive Black Holes: Prospects for LIGO-Virgo Detections

(2012)

Parameter estimation for inspiraling eccentric compact binaries including pericenter precession

Physical Review D American Physical Society (APS) 86:10 (2012) 104027

Authors:

Balázs Mikóczi, Bence Kocsis, Péter Forgács, Mátyás Vasúth

Turbulent transport and heating of trace heavy ions in hot magnetized plasmas.

Physical review letters 109:18 (2012) 185003

Authors:

M Barnes, FI Parra, W Dorland

Abstract:

Scaling laws for the transport and heating of trace heavy ions in low-frequency magnetized plasma turbulence are derived and compared with direct numerical simulations. The predicted dependences of turbulent fluxes and heating on ion charge and mass number are found to agree with numerical results for both stationary and differentially rotating plasmas. Heavy ion momentum transport is found to increase with mass, and heavy ions are found to be preferentially heated, implying a mass-dependent ion temperature for very weakly collisional plasmas and for partially ionized heavy ions in strongly rotating plasmas.

Actions for axisymmetric potentials

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 426:2 (2012) 1324-1327