Data-driven sensitivity inference for Thomson scattering electron density measurement systems.

We developed a method to infer the calibration parameters of multichannel measurement systems, such as channel variations of sensitivity and noise amplitude, from experimental data. We regard such uncertainties of the calibration parameters as dependent noise. The statistical properties of the dependent noise and that of the latent functions were modeled and implemented in the Gaussian process kernel. Based on their statistical difference, both parameters were inferred from the data. We applied this method to the electron density measurement system by Thomson scattering for the Large Helical Device plasma, which is equipped with 141 spatial channels. Based on the 210 sets of experimental data, we evaluated the correction factor of the sensitivity and noise amplitude for each channel. The correction factor varies by ≈10%, and the random noise amplitude is ≈2%, i.e., the measurement accuracy increases by a factor of 5 after this sensitivity correction. The certainty improvement in the spatial derivative inference was demonstrated.

[1]  Volker Tresp,et al.  A Bayesian Committee Machine , 2000, Neural Computation.

[2]  K. Narihara,et al.  Raman and Rayleigh Calibrations of the LHD YAG Thomson Scattering , 2007 .

[3]  G. L. Campbell,et al.  Design and operation of the multipulse Thomson scattering diagnostic on DIII‐D (invited) , 1992 .

[4]  P. Stott,et al.  Plasma Physics and Controlled Fusion Conference: Focussing on Tokamak Research , 1995 .

[5]  M. Way,et al.  NEW APPROACHES TO PHOTOMETRIC REDSHIFT PREDICTION VIA GAUSSIAN PROCESS REGRESSION IN THE SLOAN DIGITAL SKY SURVEY , 2009, 0905.4081.

[6]  R. E. Bell,et al.  Operation of the NSTX Thomson scattering system , 2002 .

[7]  Chihiro Suzuki,et al.  Development and application of real-time magnetic coordinate mapping system in the Large Helical Device , 2012 .

[8]  Oliver Stegle,et al.  Gaussian Process Robust Regression for Noisy Heart Rate Data , 2008, IEEE Transactions on Biomedical Engineering.

[9]  P. Murdin MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY , 2005 .

[10]  E. Martin,et al.  Gaussian process regression for multivariate spectroscopic calibration , 2007 .

[11]  S. Aigrain,et al.  A Gaussian process framework for modelling instrumental systematics: application to transmission spectroscopy , 2011, 1109.3251.

[12]  Jeff M. Candy,et al.  Implementation and application of two synthetic diagnostics for validating simulations of core tokamak turbulence , 2009 .

[13]  N. Davey,et al.  Photometric redshift estimation using Gaussian processes , 2009 .

[14]  E. Rodner,et al.  Automatic identification of novel bacteria using Raman spectroscopy and Gaussian processes. , 2013, Analytica chimica acta.

[15]  H. Murmann,et al.  The Thomson scattering systems of the ASDEX upgrade tokamak , 1992 .

[16]  M. Hole,et al.  Using Bayesian analysis and Gaussian processes to infer electron temperature and density profiles on the Mega-Ampere Spherical Tokamak experiment. , 2013, The Review of scientific instruments.

[17]  Youssef M. Marzouk,et al.  Improved profile fitting and quantification of uncertainty in experimental measurements of impurity transport coefficients using Gaussian process regression , 2015 .

[18]  A. W.,et al.  Journal of chemical information and computer sciences. , 1995, Environmental science & technology.

[19]  D. Robinson,et al.  Measurement of the Electron Temperature by Thomson Scattering in Tokamak T3 , 1969, Nature.

[20]  I. Yamada,et al.  Raman calibration of the LHD YAG Thomson scattering for electron-density measurements , 2003 .

[21]  Frank R. Burden,et al.  Quantitative Structure-Activity Relationship Studies Using Gaussian Processes , 2001, J. Chem. Inf. Comput. Sci..

[22]  K. Narihara,et al.  Current status of the LHD Thomson scattering system , 2012 .