Z eff spatial profiles from Bremsstrahlung emission in the near infrared spectral region

Measurements of plasma radiation in the infrared (IR) BREM_IR range (λ=978  nm , Δλ=38  nm ), at 16 horizontal lines of sight intersecting the central vertical chord of the [Frascati Tokamak Upgrade (FTU) R=0.935  m , a=0.3  m , B=4–8  T ], from z=−0.22  m below, to z=0.08  m above the equatorial pl...

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Hauptverfasser: Orsitto, F., Belforte, M. R., Brusadin, A., Giovannozzi, E., Pacella, D., May, M. J.
Format: Tagungsbericht
Sprache:eng
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Zusammenfassung:Measurements of plasma radiation in the infrared (IR) BREM_IR range (λ=978  nm , Δλ=38  nm ), at 16 horizontal lines of sight intersecting the central vertical chord of the [Frascati Tokamak Upgrade (FTU) R=0.935  m , a=0.3  m , B=4–8  T ], from z=−0.22  m below, to z=0.08  m above the equatorial plane, are performed using the detection system of the Thomson scattering apparatus [F. Orsitto et al., Appl. Opt. 34, 2712 (1995)] (TS). The measured BREM_IR intensity is equal I(z)=〈Z eff Gn e 2 /T e 1/2 〉 where 〈〉 means line average. For determining the Z eff , the Gaunt factor (G) is needed, and the Born–Elwert formula is used. The Z eff spatial profiles are determined using the plasma temperature (T e ) and density (n e ) measured by the TS, DCN interferometer, and Abel inverted intensity profiles. Z eff (r) versus time behavior in FTU discharges is presented for krypton injection experiments aimed to investigate the particle confinement behavior during strong injection of impurities.
ISSN:0034-6748
1089-7623
DOI:10.1063/1.1149462