2018
DOI: 10.1088/1741-4326/aaa6e1
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Deuterium temperature, drift velocity, and density measurements in non-Maxwellian plasmas at ASDEX Upgrade

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Cited by 26 publications
(36 citation statements)
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“…where S is the diagnostic signal, F is the fast-ion distribution function, and X are the chosen phase-space coordinates. The most commonly used and provided by FIDASIM are velocity-space weight functions F (E, p), where E and p are the fast-ion energy and pitch [13]. In addition, more complete orbit weight functions have e.g.…”
Section: Fida Weight Functionsmentioning
confidence: 99%
“…where S is the diagnostic signal, F is the fast-ion distribution function, and X are the chosen phase-space coordinates. The most commonly used and provided by FIDASIM are velocity-space weight functions F (E, p), where E and p are the fast-ion energy and pitch [13]. In addition, more complete orbit weight functions have e.g.…”
Section: Fida Weight Functionsmentioning
confidence: 99%
“…NBI can also heat preferentially in parallel or perpendicular directions. In such cases we can think of a parallel temperature T and a perpendicular temperature T ⊥ in a bi-Maxwellian velocity distribution function [13,[21][22][23][24][25]. The very large perpendicular temperature obtained by ICRF heating is sometimes called the tail temperature.…”
Section: Drifting Bi-maxwellianmentioning
confidence: 99%
“…But since the bi-Maxwellian is a 2D function, the energy spectrum and the speed distribution do not appear to be directly useful. However, the 1D projection of the bi-Maxwellian is important to understand diagnostics relying on the Doppler shift [25]. The 1D projection of the isotropic Maxwellian was given in section III based on the isotropy of the function.…”
Section: Drifting Bi-maxwellianmentioning
confidence: 99%
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