By injection of microwave power P_EC near the electron cyclotron (EC) frequency into an Ohmically heated (OH) plasma in the WT-2 tokamak after OH power is shut off, the plasma current is sustained and ramped up by the EC wave only, without OH power. Here, EC-driven current is generated by EC heating of the suprathermal electron beam in OH plasma. Further, when P_EC is injected into plasma sustained by lower-hybrid- (LH-) driven current, the plasma current and its rampup rate increase. Here, EC-driven current is generated by EC heating of the mildly relativistic electrons in LH-driven plasma
The important goal of adding to the bootstrap a fraction of non-inductive plasma current, which woul...
The important goal of adding to the bootstrap a fraction of non-inductive plasma current, which woul...
Tokamaks may be efficiently heated at electron cyclotron resonance by launching of the extraordinary...
Electron cyclotron current drive (ECCD) at the second harmonic (ω=2Ω_e) is demonstrated for two type...
The electron cyclotron (EC) system on EAST consists of four gyrotrons with a frequency of 140 GHz (s...
The electron cyclotron (EC) system on EAST consists of four gyrotrons with a frequency of 140 GHz (s...
The physics of tokamak plasmas, in which electrons are heated by electron cyclotron heating (ECH) an...
Fully non-inductive second (2nd) harmonic electron cyclotron (EC) plasma current ramp-up was demonst...
Spontaneous formation of spherical tokamak is observed during a microwave discharge at the electron ...
Plasma heating and non-inductive current drive by waves in the electron cyclotron range of frequenci...
Plasma heating and non-inductive current drive by waves in the electron cyclotron range of frequenci...
Plasma heating in existing tokamak devices by electron cyclotron waves with frequency (f) significan...
Noninductive plasma current start-up using 2nd harmonic electron cyclotron resonance heating (ECRH) ...
The existing ECWGB code which describes the quasi-optical propagation of a Gaussian beam of electron...
Electron cyclotron resonance heating (ECRH) experiments at 39 GHz with power levels similar to those...
The important goal of adding to the bootstrap a fraction of non-inductive plasma current, which woul...
The important goal of adding to the bootstrap a fraction of non-inductive plasma current, which woul...
Tokamaks may be efficiently heated at electron cyclotron resonance by launching of the extraordinary...
Electron cyclotron current drive (ECCD) at the second harmonic (ω=2Ω_e) is demonstrated for two type...
The electron cyclotron (EC) system on EAST consists of four gyrotrons with a frequency of 140 GHz (s...
The electron cyclotron (EC) system on EAST consists of four gyrotrons with a frequency of 140 GHz (s...
The physics of tokamak plasmas, in which electrons are heated by electron cyclotron heating (ECH) an...
Fully non-inductive second (2nd) harmonic electron cyclotron (EC) plasma current ramp-up was demonst...
Spontaneous formation of spherical tokamak is observed during a microwave discharge at the electron ...
Plasma heating and non-inductive current drive by waves in the electron cyclotron range of frequenci...
Plasma heating and non-inductive current drive by waves in the electron cyclotron range of frequenci...
Plasma heating in existing tokamak devices by electron cyclotron waves with frequency (f) significan...
Noninductive plasma current start-up using 2nd harmonic electron cyclotron resonance heating (ECRH) ...
The existing ECWGB code which describes the quasi-optical propagation of a Gaussian beam of electron...
Electron cyclotron resonance heating (ECRH) experiments at 39 GHz with power levels similar to those...
The important goal of adding to the bootstrap a fraction of non-inductive plasma current, which woul...
The important goal of adding to the bootstrap a fraction of non-inductive plasma current, which woul...
Tokamaks may be efficiently heated at electron cyclotron resonance by launching of the extraordinary...