Advances in neutral-beam-based diagnostics on the Madison Symmetric Torus reversed-field pinch (invited)

Innovative charge-exchange recombination spectroscopy (CHERS), motional Stark effect (MSE), and Rutherford scattering diagnostics are now in operation on the Madison Symmetric Torus (MST) reversed-field pinch (RFP). The CHERS diagnostic measures impurity ion flow and temperature, localized to 2 cm w...

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Veröffentlicht in:Review of scientific instruments 2006-10, Vol.77 (10)
Hauptverfasser: Den Hartog, D. J., Craig, D., Ennis, D. A., Fiksel, G., Gangadhara, S., Holly, D. J., Reardon, J. C., Davydenko, V. I., Ivanov, A. A., Lizunov, A. A., O’Mullane, M. G., Summers, H. P.
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Sprache:eng
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Zusammenfassung:Innovative charge-exchange recombination spectroscopy (CHERS), motional Stark effect (MSE), and Rutherford scattering diagnostics are now in operation on the Madison Symmetric Torus (MST) reversed-field pinch (RFP). The CHERS diagnostic measures impurity ion flow and temperature, localized to 2 cm with high time resolution ( ∼ 100 kHz ) . A spectral MSE diagnostic has been in use for five years, measuring ∣ B ∣ down to 0.2 T with high precision ( ∼ 2 % ) and good time resolution ( 10 kHz ) . The Rutherford scattering diagnostic has demonstrated the robustness of this technique for reliable measurement of majority (D) ion temperature, also with high time resolution. MST is a large RFP ( R = 1.5 m , a = 0.52 m ) operated at moderate current ( I p ⩽ 600 kA ) , with n e typically ( 1 – 2 ) × 10 19 m − 3 and T e , T i ⩽ 2 keV . Two compact and reliable diagnostic neutral beams are installed on MST. These beams are short pulse, intense, monoenergetic, and low divergence. The first, a neutral H beam, is used in combination with ultraviolet and visible spectroscopy to make the CHERS and MSE measurements. For CHERS, the C VI line at 343.4 nm is collected by a custom high-throughput double grating spectrometer which simultaneously records both charge-exchange and background emissions. The spectrum is analyzed using a sophisticated model derived from the Atomic Database and Analysis Structure (ADAS) package. The MSE system records the entire H α Stark spectrum; ∣ B ∣ is derived from the measured splitting of the π + and π − manifolds. Measurement of ∣ B ∣ is critical to accurate equilibrium reconstruction in the RFP. The second diagnostic beam is a 20 keV neutral He beam and is used for the Rutherford scattering measurements. A pair of neutral particle analyzers is used to record the energy spectrum of the small-angle Rutherford scattered He atoms.
ISSN:0034-6748
1089-7623
DOI:10.1063/1.2217920