Observation and characterisation of trapped electron modes in Wendelstein 7-X

Abstract In the past, quasi coherent (QC) modes were reported for nearly all tokamaks. The general definition describes modes as QC when the magnitude squared coherence is in the range of 0.3 to 0.6. QC 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, QC 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 QC modes at low wave numbers. A poloidal correlation reflectometer installed at W7-X, is able to measure low wave numbers ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mi>k</mml:mi> <mml:mo>⊥</mml:mo> </mml:msub> <mml:mtext>⩽</mml:mtext> <mml:mrow> <mml:mn>3.5</mml:mn> </mml:mrow> <mml:mstyle scriptlevel="0"/> <mml:msup> <mml:mtext>cm</mml:mtext> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> ). For medium line-averaged densities ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo>∫</mml:mo> <mml:msub> <mml:mi>n</mml:mi> <mml:mtext>e</mml:mtext> </mml:msub> <mml:mtext>⩽</mml:mtext> <mml:mrow> <mml:mn>6</mml:mn> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mn>19</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> <mml:mstyle scriptlevel="0"/> <mml:msup> <mml:mtext>m</mml:mtext> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> ) the plasma core is accessible for this diagnostic. For different magnetic configurations and plasma parameters, broad QC structures are observed in the coherence spectra. From the analysis of the rotation and the poloidal structure, these 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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Publication Details

Journal
Plasma Physics and Controlled Fusion
Published
2024-12-18
DOI
https://doi.org/10.1088/1361-6587/ada0db
Citations
5
Primary Topic
Magnetic confinement fusion research
Type
article
Field-Weighted Citation Impact
3.30

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article

Observation and characterisation of trapped electron modes in Wendelstein 7-X

Haoming Xiang, L. Salazar, S. Heuraux, J. Geiger et al.
5 citations
Plasma Physics and Controlled Fusion
Magnetic confinement fusion research
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article

Observation and characterisation of trapped electron modes in Wendelstein 7-X

Haoming Xiang, L. Salazar, S. Heuraux, J. Geiger, J. H. E. Proll, A. Langenberg, A. Krämer-Flecken, R. Sabot, N. Pablant, G. Weir, K. Rahbarnia, G. Fuchert, S. Vaz Mendes, T. Windisch, A. Knieps, H. Thomsen, P. Costello, E. Pasch, H. M. Smith
article en
5 citations

Abstract

Abstract In the past, quasi coherent (QC) modes were reported for nearly all tokamaks. The general definition describes modes as QC when the magnitude squared coherence is in the range of 0.3 to 0.6. QC 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, QC 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 QC modes at low wave numbers. A poloidal correlation reflectometer installed at W7-X, is able to measure low wave numbers ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mi>k</mml:mi> <mml:mo>⊥</mml:mo> </mml:msub> <mml:mtext>⩽</mml:mtext> <mml:mrow> <mml:mn>3.5</mml:mn> </mml:mrow> <mml:mstyle scriptlevel="0"/> <mml:msup> <mml:mtext>cm</mml:mtext> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> ). For medium line-averaged densities ( <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo>∫</mml:mo> <mml:msub> <mml:mi>n</mml:mi> <mml:mtext>e</mml:mtext> </mml:msub> <mml:mtext>⩽</mml:mtext> <mml:mrow> <mml:mn>6</mml:mn> <mml:mo>×</mml:mo> <mml:msup> <mml:mn>10</mml:mn> <mml:mrow> <mml:mn>19</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> <mml:mstyle scriptlevel="0"/> <mml:msup> <mml:mtext>m</mml:mtext> <mml:mrow> <mml:mo>−</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> ) the plasma core is accessible for this diagnostic. For different magnetic configurations and plasma parameters, broad QC structures are observed in the coherence spectra. From the analysis of the rotation and the poloidal structure, these 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.

Plasma Physics and Controlled FusionVol. 67(2)
Forschungszentrum Jülich (DE), Commissariat à l'Énergie Atomique et aux Énergies Alternatives (FR), Princeton Plasma Physics Laboratory (US), CEA Cadarache (FR), Max Planck Institute for Plasma Physics - Greifswald (DE), Université de Lorraine (FR)
EUROfusion, European Commission, Euratom Research and Training Programme
Openalex Percentile: Top 6%
Magnetic confinement fusion research
3.30
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