1996
DOI: 10.1088/0741-3335/38/11/004
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Ordinary-mode reflectometry: modification of the scattering and cut-off responses due to the shape of localized density fluctuations

Abstract: Ordinary wave reflectometry in a plasma containing a localized density perturbation is studied with a one-dimensional (1D) model. The phase response is studied as a function of the wavenumber and position of the perturbation. It is shown that it strongly depends upon the perturbation shape and size. For a small perturbation wavenumber, the response is due to the oscillation of the cut-off layer. For larger wavenumbers, two regimes of resonant Bragg scattering are found: for a broad perturbation, the phase resp… Show more

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Cited by 59 publications
(72 citation statements)
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“…32 The phase of the reflectometry signal is inferred directly from the radial structure of the electric field, which is illustrated in Fig. 4 Under the Born approximation valid for low levels of the density fluctuations, it was shown in previous works [33][34][35] that the phase fluctuations could be retrieved directly from the integral of the density fluctuations along the radial line-of-sight…”
Section: B Comparison Between O-mode and X-mode Resultsmentioning
confidence: 98%
“…32 The phase of the reflectometry signal is inferred directly from the radial structure of the electric field, which is illustrated in Fig. 4 Under the Born approximation valid for low levels of the density fluctuations, it was shown in previous works [33][34][35] that the phase fluctuations could be retrieved directly from the integral of the density fluctuations along the radial line-of-sight…”
Section: B Comparison Between O-mode and X-mode Resultsmentioning
confidence: 98%
“…10(a) and 10(b)) according the plasma density which modifies the distance between the antenna and the cut-off layer, and modifies as well the influence of the density fluctuations which are less disturbing on the phase signal as the density gradient is getting steeper. 22 Before the first cut-off, the antenna coupling signal is clearly visible at approximately -35 dB below the highest plasma echo. Above 62 GHz, multi-reflections can be distinguished in Fig.…”
Section: Reflectometry and Lhcd Launcher Arrangementmentioning
confidence: 97%
“…EC codes: In the frequency range of electron cyclotron heating, the Helmholtz solvers were used for diagnostics (Fanack et al 1996;Mazzucato 1998) a long time ago. Until recently, the ray tracing method was estimated to be enough to study a beam propagation in ITER plasmas (Prater et al 2008), but it is clear now that the density fluctuations have to be included , and, for these studies, full-wave codes are required for the frequency range of electron cyclotron heating or current drive (Sysoeva et al , 2015.…”
Section: Heating Simulationmentioning
confidence: 99%
“…In the first case, all spatial scales are present, and the scattered is more or less isotropic after averaging. Then, part of the spectrum is truncated and, as a consequence, an anisotropy appears in the scattered field pattern, according to the Bragg rule (see (Fanack et al 1996)). In the last one, only forward scattering is possible, showing a narrow lobe for the scattered wave emission.…”
Section: Conclusion and New Developmentsmentioning
confidence: 99%