The Er×B flow shear is simulated with a fully kinetic five-dimensional neoclassical Monte Carlo simulation for JET and ASDEX Upgrade plasma edge conditions. Here, Er is the radial electric field and B is the magnetic field. It is shown that high enough shear for turbulence suppression can be driven at the Low (L) to High (H) transition conditions by pure neoclassical effects including ion orbit losses. Simulations indicate higher threshold shear for ASDEX Upgrade than for JET. Shear values are compared to different models and experimental results of critical shear, and isotope effect on shear is discussed. Formation of an internal transport barrier in FT-2 in the presence of lower hybrid waves is also studied
Monte Carlo ion simulation and semi‐analytical calculation of the neoclassical radial current balanc...
Transport barriers with strong density and temperature gradients can appear in regions with large ve...
One of the principal problems en route to a fusion reactor is that of insufficient plasma confinemen...
The Er×B flow shear is simulated with a fully kinetic five-dimensional neoclassical Monte Carlo simu...
Er×B flow shear is simulated with a fully kinetic five-dimensional neoclassical Monte Carlo simulati...
Er×B flow shear is simulated with a fully kinetic five-dimensional neoclassical Monte Carlo simulati...
Monte Carlo ion simulation based on neoclassical radial current balance near edge in a divertor toka...
Monte Carlo ion simulation based on neoclassical radial current balance near edge in a divertor toka...
Monte Carlo ion simulation based on neoclassical radial current balance in a divertor tokamak gives ...
Monte Carlo ion simulation based on neoclassical radial current balance in a divertor tokamak gives ...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
The radial electric field E<sub>r</sub> at the tokamak plasma edge is simulated both with a two-dime...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
Monte Carlo ion simulation and semi‐analytical calculation of the neoclassical radial current balanc...
Monte Carlo ion simulation and semi‐analytical calculation of the neoclassical radial current balanc...
Transport barriers with strong density and temperature gradients can appear in regions with large ve...
One of the principal problems en route to a fusion reactor is that of insufficient plasma confinemen...
The Er×B flow shear is simulated with a fully kinetic five-dimensional neoclassical Monte Carlo simu...
Er×B flow shear is simulated with a fully kinetic five-dimensional neoclassical Monte Carlo simulati...
Er×B flow shear is simulated with a fully kinetic five-dimensional neoclassical Monte Carlo simulati...
Monte Carlo ion simulation based on neoclassical radial current balance near edge in a divertor toka...
Monte Carlo ion simulation based on neoclassical radial current balance near edge in a divertor toka...
Monte Carlo ion simulation based on neoclassical radial current balance in a divertor tokamak gives ...
Monte Carlo ion simulation based on neoclassical radial current balance in a divertor tokamak gives ...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
The radial electric field E<sub>r</sub> at the tokamak plasma edge is simulated both with a two-dime...
The radial electric field Er at the tokamak plasma edge is simulated both with a two-dimensional (2D...
Monte Carlo ion simulation and semi‐analytical calculation of the neoclassical radial current balanc...
Monte Carlo ion simulation and semi‐analytical calculation of the neoclassical radial current balanc...
Transport barriers with strong density and temperature gradients can appear in regions with large ve...
One of the principal problems en route to a fusion reactor is that of insufficient plasma confinemen...