Robotic calibration of the motional Stark effect diagnostic on Alcator C-Mod

被引:11
作者
Mumgaard, Robert T. [1 ]
Scott, Steven D. [2 ]
Ko, Jinseok [3 ]
机构
[1] MIT, Plasma Sci & Fus Ctr, Cambridge, MA 02139 USA
[2] Princeton Plasma Phys Lab, Princeton, NJ 08543 USA
[3] Natl Fus Res Inst, Taejon 305806, South Korea
关键词
RADIAL ELECTRIC-FIELD; CURRENT PROFILES; TOKAMAK; DESIGN; TFTR;
D O I
10.1063/1.4873332
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
The capability to calibrate diagnostics, such as the Motional Stark Effect (MSE) diagnostic, without using plasma or beam-into-gas discharges will become increasingly important on next step fusion facilities due to machine availability and operational constraints. A robotic calibration system consisting of a motorized three-axis positioning system and a polarization light source capable of generating arbitrary polarization states with a linear polarization angle accuracy of < 0.05 degrees has been constructed and has been used to calibrate the MSE diagnostic deployed on Alcator C-Mod. The polarization response of the complex diagnostic is shown to be fully captured using a Fourier expansion of the detector signals in terms of even harmonics of the input polarization angle. The system's high precision robotic control of position and orientation allow it to be used also to calibrate the geometry of the instrument's view. Combined with careful measurements of the narrow bandpass spectral filters, this system fully calibrates the diagnostic without any plasma discharges. The system's high repeatability, flexibility, and speed has been exploited to quantify several systematics in the MSE diagnostic response, providing a more complete understanding of the diagnostic performance. (C) 2014 AIP Publishing LLC.
引用
收藏
页数:12
相关论文
共 30 条
[1]  
Beals D., 2005, P 21 IEEE NPSS S FUS, P1
[2]   An integrated charge exchange recombination spectroscopy/beam emission spectroscopy diagnostic for Alcator C-Mod tokamak [J].
Bespamyatnov, I. O. ;
Rowan, W. L. ;
Liao, K. T. ;
Granetz, R. S. .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2010, 81 (10)
[3]   AUTOMATIC-MEASUREMENT OF THE STOKES VECTOR OF LIGHT [J].
BOYER, GR ;
LAMOUROUX, BF ;
PRADE, BS .
APPLIED OPTICS, 1979, 18 (08) :1217-1219
[4]   A motional Stark effect instrument to measure q(R) on the C-mod tokamak [J].
Bretz, N ;
Simon, D ;
Parsells, R ;
Bravenec, R ;
Rowan, W ;
Eisner, N ;
Sampsell, M ;
Yuh, H ;
Marmar, E ;
Terry, J .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2001, 72 (01) :1012-1014
[5]  
Condon E. U., 1951, The Theory of Atomic Spectra, V2nd
[6]   The MAST motional Stark effect diagnostic [J].
Conway, N. J. ;
De Bock, M. F. M. ;
Michael, C. A. ;
Walsh, M. J. ;
Carolan, P. G. ;
Hawkes, N. C. ;
Rachlew, E. ;
McCone, J. F. G. ;
Shibaev, S. ;
Wearing, G. .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2010, 81 (10)
[7]   Design of the motional Stark effect diagnostic in FTU [J].
De Angelis, R ;
Sarkissian, A ;
Segre, SE ;
Tartoni, N ;
Zanza, V .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2001, 72 (01) :1015-1017
[8]   Atomic models for the motional Stark effect diagnostic [J].
Gu, M. F. ;
Holcomb, C. T. ;
Jayakuma, R. J. ;
Allen, S. L. .
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 2008, 41 (09)
[9]   Design of the joint European torus motional Stark effect diagnostic [J].
Hawkes, NC ;
Blackler, K ;
Viaccoz, B ;
Wilson, CH ;
Migozzi, JB ;
Stratton, BC .
REVIEW OF SCIENTIFIC INSTRUMENTS, 1999, 70 (01) :894-897
[10]   Status of the ITER neutral beam injection system (invited) [J].
Hemsworth, R. S. ;
Tanga, A. ;
Antoni, V. .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2008, 79 (02)