NONLINEAR-OPTICAL EFFECTS IN RAMAN CALIBRATIONS OF A THOMSON SCATTERING SYSTEM

被引:4
作者
BASSAN, M [1 ]
GIUDICOTTI, L [1 ]
PASQUALOTTO, R [1 ]
机构
[1] UNIV PADUA, DIPARTIMENTO INGN ELETTR, I-35131 PADUA, ITALY
关键词
RAMAN SCATTERING; THOMSON SCATTERING; PLASMA DIAGNOSTICS;
D O I
10.1364/AO.32.005313
中图分类号
O43 [光学];
学科分类号
070207 ; 0803 ;
摘要
We present an investigation of the occurrence of stimulated Raman scattering and other nonlinear optical effects during Raman calibrations of Thomson scattering diagnostic systems for magnetic fusion plasmas. When these effects take place, the intensity of the Raman lines is unpredictable, and the calibrations are impossible. In this research Raman scattering from H-2 and D2 at filling pressures up to 1 atm has been experimentally investigated using the Thomson scattering system of the ETA-BETA II reversed field pinch device. Stimulated Raman Stokes light has been observed at filling pressures above 230 and 500 mbars for H-2 and D2, respectively, for input laser pulses of 8 J and 30 ns (FWHM) duration. Evidence has been found that the stimulated Raman light does not originate from the observed scattering volume but is detected as light diffused into the vacuum chamber. To explain these results, the Raman gain and the intensity of the stimulated Raman light are calculated, taking into account the multimode structure of the laser beam. We find that significant power conversion from the input laser beam to the Stokes wave takes place near the output window of the vacuum chamber. Part of this radiation is diffused back into the machine, and this part is detected as superimposed on the spontaneous Raman signal. Finally we discuss the Raman calibrations in RFX, a larger plasma device in which the Raman medium will be N2 at a temperature up to 350-degrees-C, and show that a filling pressure of 100 mbar gives a sufficient calibration signal, avoiding any nonlinear effect.
引用
收藏
页码:5313 / 5323
页数:11
相关论文
共 46 条
[1]  
ANTONI V, 1989, PLASMA PHYS CONTROLL, V2, P661
[2]   APPARATUS FOR MULTIPOINT THOMSON SCATTERING MEASUREMENTS IN THE ETA-BETA-II REVERSED FIELD PINCH EXPERIMENT [J].
BASSAN, M ;
BUFFA, A ;
GIUDICOTTI, L .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1985, 56 (05) :1027-1029
[3]   AUTOMATIC LASER-BEAM ALIGNMENT FOR A THOMSON SCATTERING SYSTEM [J].
BASSAN, M ;
FLORA, F ;
GIUDICOTTI, L .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1988, 59 (08) :1482-1484
[4]   DEVELOPMENT OF A MULTIPOINT THOMSON SCATTERING SYSTEM FOR A LARGE REVERSED FIELD PINCH EXPERIMENT [J].
BASSAN, M ;
PASQUALOTTO, R ;
SARDELLA, A ;
GIUDICOTTI, L .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1990, 61 (10) :2846-2848
[5]   CONTROLLED STIMULATED RAMAN AMPLIFICATION AND OSCILLATION IN HYDROGEN GAS [J].
BLOEMBER.N ;
BRET, G ;
LALLEMAN.P ;
PINE, A ;
SIMOVA, P .
IEEE JOURNAL OF QUANTUM ELECTRONICS, 1967, QE 3 (05) :197-+
[6]   16-MU-M GENERATION BY CO2-PUMPED ROTATIONAL RAMAN-SCATTERING IN H-2 [J].
BYER, RL ;
TRUTNA, WR .
OPTICS LETTERS, 1978, 3 (04) :144-146
[7]   16-MU-M SOURCE FOR LASER ISOTOPE ENRICHMENT [J].
BYER, RL .
IEEE JOURNAL OF QUANTUM ELECTRONICS, 1976, 12 (11) :732-733
[8]  
Carslaw H.S., 1959, CONDUCTION HEAT SOLI
[9]   DICKE NARROWING AND COLLISIONAL BROADENING OF S0(O) AND S0(1) RAMAN LINE OF H2 [J].
COOPER, VG ;
MAY, AD ;
HARA, EH ;
KNAPP, HFP .
CANADIAN JOURNAL OF PHYSICS, 1968, 46 (18) :2019-+
[10]   INTERFEROMETRIC MEASUREMENT OF LINE WIDTHS AND FREQUENCIES OF S0(O) AND SO(I) ROTATIONAL RAMAN LINES OF H2 [J].
COOPER, VG ;
MAY, AD ;
GUPTA, BK .
CANADIAN JOURNAL OF PHYSICS, 1970, 48 (06) :725-+