Abstract Abstract. In the past, quasi coherent modes were reported for nearly all tokamaks.
The general definition describes modes as quasi coherent when the magnitude squared
coherence is in the range of 0.3 to 0.6. Quasi coherent modes are observed in the
plasma core as well as in the plasma edge and can have quite different physical origins.
The one in the core are observed in plasmas with low collisionality, where the electron
temperature exceeds the ion temperature in the plasma core. This is the case for
electron cyclotron heating in general. The origin of these modes are electrons trapped
within a magnetic mirror, as reported in the past from various fusion devices. The
so-called trapped-electron modes (TEMs) belong to drift wave instabilities and can be
destabilized by electron-temperature gradients in the plasma core. From the diagnostic
point of view, quasi coherent modes appear as fluctuations in electron density and
temperature. Therefore, the microwave reflectometer is very well suited to monitor
these modes.
This paper describes experiments, conducted at the Wendelstein 7-X stellarator (W7-
X), which aim at detecting quasi coherent modes at low wave numbers. A Poloidal
Correlation Reflectometer (PCR) installed at W7-X, is able to
R measure low wave
numbers (k⊥ ≤ 3.5 cm−1 ). For medium line-averaged densities ( ne ≤ 6 × 1019 m−2 )
the plasma core is accessible for this diagnostic. For different magnetic configurations
and plasma parameters, broad quasi-coherent structures are observed in the coherence
spectra. From the analysis of the rotation and the poloidal structure, these quasi
coherent (QC) modes show the properties of electron-temperature-gradient driven
TEMs. A linear relation between the mode velocity and the rotation frequency is
found. The relation is uniform and confirms the nature of QC-mode observation as
TEM in tokamaks, too.
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