2002
DOI: 10.1590/s0103-97332002000100005
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Cited by 5 publications
(5 citation statements)
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“…One was an EMI 9635B single channel photomultiplier, at 1000 V. A sodium salicilate scintillator between the exit slit and the photomultiplier makes the conversion of VUV to visible photons (to which the photomultiplier is sensitive). The other was a multichannel detector consisting of a MCP plate coupled to a CCD device specially mounted for our spectrometer by McPherson Inc. [3]. When using the multichannel detector, the scintillator is taken away.…”
Section: Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…One was an EMI 9635B single channel photomultiplier, at 1000 V. A sodium salicilate scintillator between the exit slit and the photomultiplier makes the conversion of VUV to visible photons (to which the photomultiplier is sensitive). The other was a multichannel detector consisting of a MCP plate coupled to a CCD device specially mounted for our spectrometer by McPherson Inc. [3]. When using the multichannel detector, the scintillator is taken away.…”
Section: Methodsmentioning
confidence: 99%
“…The plasma used for the calibration and measurements was produced in the NOVA-UNICAMP tokamak [3], [4]. This is a small tokamak with 30-cm major radius, 6-cm minor radius, and iron core transformer for ohmic heating.…”
Section: Introductionmentioning
confidence: 99%
“…In practice, the calculation of τ P values itself are not necessary, being sufficient to calculate the ratio between confinement times for different hydrogen emissions, and to find electron temperatures and densities values that satisfy the relationship: Now we have two independent equations which allow us to find the T e and n e parameters. The equations (4) and (5) show that the ratios between particle confinement times depends only on the measured brightness and its respective R factors, avoiding difficulties inherent to the determination of N e , l and r 0 parameters of equation (1).…”
Section: Theoretical Modelmentioning
confidence: 99%
“…In this work we present a diagnostic method used to determine the local electron temperature (T e ) and density (n e ) in the NOVA-UNICAMP tokamak (NUt) plasma using visible spectroscopy, which has the advantage to be a passive method. The NOVA-UNICAMP [1] is a small iron core tokamak with major radius R = 0.30 m, plasma radius a = 0.06 m, toroidal field B T = 0.8 T and characteristic plasma current of I P = 10 kA.…”
Section: Introductionmentioning
confidence: 99%
“…The development of diagnostic tools and methods for measurements of plasma parameters, like temperatures, densities, and confinement times, is an important matter in plasma physics. In previous works [1][2][3], we have used spectral emissions originating from neutral hydrogen and C 1+ (CII) ions in order to measure the electron densities and temperatures at the edge of NOVA-UNICAMP tokamak plasma [4]. The method developed in [3] uses a well-known relationship between the particle flux and the photon flux emitted by an ion species [5][6][7] combined with ionizations per photon atomic data provided by the atomic data and analysis structure (ADAS) database [8].…”
Section: Introductionmentioning
confidence: 99%