A real-time Alfvén eigenmode (AE) controller is designed and implemented for the first time in DIII-D. The experimental test consists of two parts: (i) open-loop and feedback control using neutral beam power as an actuator and (ii) open-loop control using electron cyclotron heating (ECH) as an actuator. Part (i) demonstrates the feasibility of varying neutral beam power injected into plasma to control overall AE amplitude as well as the successful application of real-time electron cyclotron emission (ECE) as the process controller's AE amplitude sensor. The temporal evolution of AE amplitude at a specific radial location has also been controlled by selecting a subset of the radial ECE array. Part (ii) finds a complicated dependence of AE ev...
Alfvén cascades (ACs) and beta-induced Alfvén eigenmodes (BAEs) have been studied in the ASDEX Upgra...
ASDEX Upgrade has a large variety of technical systems, heating and fuelling as well as digital ...
The spatial structure of toroidal Alfvén eigenmodes and reversed shear Alfvén eigenmodes in DIII-D i...
A recent DIII-D experiment investigating the impact of electron cyclotron heating (ECH) on neutral b...
OAK A271 INCREASED STABLE BETA IN DIII-D BY SUPPRESSION OF A NEOCLASSICAL TEARING MODE USING ELECTRO...
Neutral beam injection into reversed magnetic shear DIII-D plasmas produces a variety of Alfvénic ac...
A first-ever demonstration of controlling power and torque injection through time evolution of neutr...
The stability and performance of tokamak plasmas are limited by instabilities such as neoclassical t...
A demonstration of real-time feedback control for autonomous tracking and stabilization of m/n = 2/1...
Initial experiments on heating and current drive using second harmonic electron cyclotron heating (E...
The stability properties of Alfvén Eigenmodes (AEs) are investigated directly using external antenna...
OAK A271 RECENT DEVELOPMENTS ON THE 110 GHZ ELECTRON CYCLOTRON INSTALLATION ON THE DIII-D TOKAMAK. S...
Understanding the interaction between wave excitation and damping is essential in the advancement of...
A real-time feedback control system has been developed that finds, tracks, suppresses and/or stabili...
Alfvén waves are electromagnetic perturbations inherent to magnetized plasmas that can be driven uns...
Alfvén cascades (ACs) and beta-induced Alfvén eigenmodes (BAEs) have been studied in the ASDEX Upgra...
ASDEX Upgrade has a large variety of technical systems, heating and fuelling as well as digital ...
The spatial structure of toroidal Alfvén eigenmodes and reversed shear Alfvén eigenmodes in DIII-D i...
A recent DIII-D experiment investigating the impact of electron cyclotron heating (ECH) on neutral b...
OAK A271 INCREASED STABLE BETA IN DIII-D BY SUPPRESSION OF A NEOCLASSICAL TEARING MODE USING ELECTRO...
Neutral beam injection into reversed magnetic shear DIII-D plasmas produces a variety of Alfvénic ac...
A first-ever demonstration of controlling power and torque injection through time evolution of neutr...
The stability and performance of tokamak plasmas are limited by instabilities such as neoclassical t...
A demonstration of real-time feedback control for autonomous tracking and stabilization of m/n = 2/1...
Initial experiments on heating and current drive using second harmonic electron cyclotron heating (E...
The stability properties of Alfvén Eigenmodes (AEs) are investigated directly using external antenna...
OAK A271 RECENT DEVELOPMENTS ON THE 110 GHZ ELECTRON CYCLOTRON INSTALLATION ON THE DIII-D TOKAMAK. S...
Understanding the interaction between wave excitation and damping is essential in the advancement of...
A real-time feedback control system has been developed that finds, tracks, suppresses and/or stabili...
Alfvén waves are electromagnetic perturbations inherent to magnetized plasmas that can be driven uns...
Alfvén cascades (ACs) and beta-induced Alfvén eigenmodes (BAEs) have been studied in the ASDEX Upgra...
ASDEX Upgrade has a large variety of technical systems, heating and fuelling as well as digital ...
The spatial structure of toroidal Alfvén eigenmodes and reversed shear Alfvén eigenmodes in DIII-D i...