Hauptseite > Publikationsdatenbank > Feasibility of ECE measurements using Hilbert-transform spectral analysis > print |
001 | 154254 | ||
005 | 20240610121117.0 | ||
024 | 7 | _ | |2 WOS |a WOS:000336947200007 |
037 | _ | _ | |a FZJ-2014-03630 |
041 | _ | _ | |a English |
082 | _ | _ | |a 530 |
100 | 1 | _ | |0 P:(DE-Juel1)130621 |a Divin, Yuri |b 0 |e Corresponding Author |u fzj |
245 | _ | _ | |a Feasibility of ECE measurements using Hilbert-transform spectral analysis |
260 | _ | _ | |a La Grange Park, Ill. |b American Nuclear Society |c 2014 |
336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1403872978_4389 |2 PUB:(DE-HGF) |
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336 | 7 | _ | |a ARTICLE |2 BibTeX |
336 | 7 | _ | |a JOURNAL_ARTICLE |2 ORCID |
336 | 7 | _ | |a article |2 DRIVER |
520 | _ | _ | |a Electron cyclotron emission (ECE) from hot tokamak plasmas is recognized nowadays as a very informative diagnostic of main plasma parameters. Among several instruments developed to measure ECE, only a Martin-Puplett interferometer operates in a broadband frequency range of ECE from 70 to 1000 GHz. To derive the absolute radiation temperature of the plasma, a total measurement system, including front-end radiation collection, a transmission line, and the interferometer, is calibrated using a hot/cold calibration source. It takes a long time to calibrate the ECE system because of the high values of the noise equivalent power (NEP). A new technique, Hilbert-transform spectral analysis, is proposed for ITER plasma ECE spectral measurements. The operation principle, characteristics, and advantages of the corresponding Hilbert-transform spectrum analyzer (HTSA) based on a high-Tc Josephson detector are described. Because of the lower NEP values of the Josephson detector, this spectrum analyzer might demonstrate shorter calibration times than those for the Martin-Puplett interferometer. Because of a principal difference between Fourier and Hilbert transforms, the HTSA might have an additional advantage in retrieving harmonic ECE radiation from a continuous thermal background. |
536 | _ | _ | |0 G:(DE-HGF)POF2-423 |a 423 - Sensorics and bioinspired systems (POF2-423) |c POF2-423 |f POF II |x 0 |
700 | 1 | _ | |0 P:(DE-HGF)0 |a Pandya, H. K. B. |b 1 |
773 | _ | _ | |0 PERI:(DE-600)2132501-7 |p 399-405 3 |t Fusion science and technology |v 65 |x 0748-1896 |y 2014 |
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914 | 1 | _ | |y 2014 |
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