2014
DOI: 10.1088/1009-0630/16/4/02
|View full text |Cite
|
Sign up to set email alerts
|

Density Profile and Fluctuation Measurements by Microwave Reflectometry on EAST

Abstract: A microwave reflectometry system operating in the V-band frequency with extraordinary mode polarization has been developed on the EAST tokamak. The reflectometry system, using a voltage-controlled oscillator (VCO) source driven by an arbitrary waveform generator with high temporal resolution, can operate for the density profile measurement. The result of the bench test shows that the output frequency of the VCO has a linear dependence on time. The dispersion of reflectometry system is determined and reported i… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
44
0

Year Published

2016
2016
2024
2024

Publication Types

Select...
10

Relationship

0
10

Authors

Journals

citations
Cited by 82 publications
(44 citation statements)
references
References 14 publications
0
44
0
Order By: Relevance
“…[24] Figure 7 displays two density profiles measured by the microwave reflectometry before and during the ELM supersession. [25] The density gradient in the pedestal is softened during ELM suppression compared with that before, which could be attributed to the enhanced pedestal transport. These results indicate that ELMs can be suppressed due to the changed pedestal transport by impurities.…”
Section: Influence Of Impurity On the Elmmentioning
confidence: 88%
“…[24] Figure 7 displays two density profiles measured by the microwave reflectometry before and during the ELM supersession. [25] The density gradient in the pedestal is softened during ELM suppression compared with that before, which could be attributed to the enhanced pedestal transport. These results indicate that ELMs can be suppressed due to the changed pedestal transport by impurities.…”
Section: Influence Of Impurity On the Elmmentioning
confidence: 88%
“…The electron density was measured by reflectometry (Refl). [27][28][29] The electron temperature was measured by a Michelson interferometer (MI), 30 a heterodyne radiometer system (HRS), 31 and Thomson scattering (TS). 32 The ion temperature was measured by charge exchange recombination spectroscopy (CXRS).…”
Section: Setup Of the Simulationsmentioning
confidence: 99%
“…In this work, we carried out the linear stability analysis of equilibrium 1 with relatively lower Z eff ~ 2.8 at about 1880 ms, which is operated with line-averaged density <n e > ~ 3.510 19 Figure 2 shows the electron density, electron temperature, total plasma pressure and current density profiles of the two equilibria. The edge electron density profiles are measured by microwave reflectometer system [34] which is located at low-field side midplane. The electron temperature profiles are obtained from Thomson Scattering system [35,36].…”
Section: Extended Mhd Model and Equilibriamentioning
confidence: 99%