2008
DOI: 10.1063/1.2909160
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The WEGA Stellarator: Results and Prospects

Abstract: Abstract. In this article an overview is given on results from magnetic flux surface measurements, applied ECR heating scenarios for 2.45GHz and 28GHz, fluctuation and transport studies and plasma edge biasing experiments performed in the WEGA stellarator. Examples for the development of new diagnostics and the machine control system are given that will be used at Wendelstein 7-X stellarator, which is currently under construction in Greifswald.

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Cited by 14 publications
(10 citation statements)
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“…Similar visualization techniques have been used before, e.g. to calibrate the vertical field coils in TEXTOR [5], to investigate the stability of the rotational transform for high field experiments in W7-AS [6] or to prove the existence of magnetic surfaces in CNT [7]. However, the exact 3-dimensional structure and position of the luminescent trace as a visualization of the magnetic field line was not yet measured.…”
Section: Recent Experimental Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Similar visualization techniques have been used before, e.g. to calibrate the vertical field coils in TEXTOR [5], to investigate the stability of the rotational transform for high field experiments in W7-AS [6] or to prove the existence of magnetic surfaces in CNT [7]. However, the exact 3-dimensional structure and position of the luminescent trace as a visualization of the magnetic field line was not yet measured.…”
Section: Recent Experimental Resultsmentioning
confidence: 99%
“…WEGA is a classical five period (m = 5) and l = 2 stellarator with a major radius of R = 72 cm, a minor radius of the vessel of r = 19 cm and a maximum plasma radius of a ≈ 11 cm [1]. Furthermore, WEGA is equipped with a set of vertical field coils, which are used for adjusting the radial position of the plasma and for varying the magnetic shear.…”
Section: Introductionmentioning
confidence: 99%
“…In the first one the spatial position of the toroidally and poloidally circulating electron beam is detected electrically by measuring directly the electric current by means of moveable (electrostatic) probes or wire frames [8][9][10][11]. The second group comprises indirect optical detection methods of the electron beam, either by interaction with a background gas in the plasma vacuum vessel or by the excitation of a fluorescent detector rod [12][13][14][15][16][17][18] intersecting the magnetic field lines and hence generating a Poincaré plot. In addition, if the electron beam is exposed to a highly diluted background gas such as argon, nitrogen or hydrogen the whole three-dimensional structure of a field line is visible due to the inelastic collisional excitation.…”
Section: Methodsmentioning
confidence: 99%
“…This was attributed to elastic deformations of the non-planar field coils [6]. The WEGA stellarator had large n/m = 1/3 and n/m = 1/4 island chains present and was able to image island chains with polodial mode numbers up to m = 9 [7]. The error field was attributed to mis-alignments between the helix and toroidal field coils.…”
Section: Introductionmentioning
confidence: 99%