In a burning plasma, fusion-born α particles are the dominant source of heating. In such conditions, the deuterium and tritium ion energy distribution deviates from the expected thermal Maxwellian distribution
The triton distribution function during ion cyclotron range of frequency (ICRF) waves injection in D...
A series of thin glass-shell shock-driven DT gas-filled capsule implosions was conducted at the OME...
Auxiliary plasma heating by radio-frequency waves is a usual procedure in the modern tokamaks. In th...
We investigate the effects of non-equilibrium particle distributions resulting from rapid deuterium-...
Plasmas for thermonuclear fusion contain a highly non-thermal population of fast ions which may carr...
The energy balance in a thermonuclear reacting plasma containing deuterium and tritium has been disc...
“This document is intended for publication in the open literature. It is made available on the under...
An experiment at the Joint European Torus (JET) has demonstrated clear self-heating of a deuterium-t...
The Tomamak Fusion Test reactor has performed initial high-power experiments with the plasma fueled ...
We argue that the Maxwellian approximation can essentially underestimate the rates of some nuclear r...
In fusion devices measurements of the radiation temperature T{sub r} ({omega}, k) near the electron ...
During the burn of DT (Deuterium-Tritium) fuel in ICF (Inertial Confinement Fusion) target, the ener...
At the beginning of thermonuclear ignition in fusion plasma, the bremsstrahlung radiation is dominan...
Inclusion of inverse Compton effects in the calculation of deuterium-deuterium burn under the extrem...
The velocity distribution functions of the newly born (t = 0) charged fusion products of tokamak dis...
The triton distribution function during ion cyclotron range of frequency (ICRF) waves injection in D...
A series of thin glass-shell shock-driven DT gas-filled capsule implosions was conducted at the OME...
Auxiliary plasma heating by radio-frequency waves is a usual procedure in the modern tokamaks. In th...
We investigate the effects of non-equilibrium particle distributions resulting from rapid deuterium-...
Plasmas for thermonuclear fusion contain a highly non-thermal population of fast ions which may carr...
The energy balance in a thermonuclear reacting plasma containing deuterium and tritium has been disc...
“This document is intended for publication in the open literature. It is made available on the under...
An experiment at the Joint European Torus (JET) has demonstrated clear self-heating of a deuterium-t...
The Tomamak Fusion Test reactor has performed initial high-power experiments with the plasma fueled ...
We argue that the Maxwellian approximation can essentially underestimate the rates of some nuclear r...
In fusion devices measurements of the radiation temperature T{sub r} ({omega}, k) near the electron ...
During the burn of DT (Deuterium-Tritium) fuel in ICF (Inertial Confinement Fusion) target, the ener...
At the beginning of thermonuclear ignition in fusion plasma, the bremsstrahlung radiation is dominan...
Inclusion of inverse Compton effects in the calculation of deuterium-deuterium burn under the extrem...
The velocity distribution functions of the newly born (t = 0) charged fusion products of tokamak dis...
The triton distribution function during ion cyclotron range of frequency (ICRF) waves injection in D...
A series of thin glass-shell shock-driven DT gas-filled capsule implosions was conducted at the OME...
Auxiliary plasma heating by radio-frequency waves is a usual procedure in the modern tokamaks. In th...
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