Introduction to Integrated Data Analysis
- R. Fischer
Max-Planck-Institut für Plasmaphysik, Garching EURATOM Association
Frascati, Mar 26-28, 2012
7th Workshop on Fusion Data Processing, Validation and Analysis
Introduction to Integrated Data Analysis R. Fischer - - PowerPoint PPT Presentation
7 th Workshop on Fusion Data Processing, Validation and Analysis Introduction to Integrated Data Analysis R. Fischer Max-Planck-Institut fr Plasmaphysik, Garching EURATOM Association Frascati, Mar 26-28, 2012 Outline Why do we need
Max-Planck-Institut für Plasmaphysik, Garching EURATOM Association
7th Workshop on Fusion Data Processing, Validation and Analysis
➢ Why do we need Integrated Data Analysis (IDA)? ➢ Implementation of IDA ➢ Applications at ➢ W7-AS ➢ JET ➢ TJ-II stellarator ➢ ASDEX Upgrade tokamak ➢ Integrated Diagnostics Design (IDD) is closely related to IDA
→ talk A. Dinklage
Different measurement techniques (diagnostics: LIB, DCN, ECE, TS, REF, ...) for the same quantities (ne, Te, …) and parametric entanglement in data analysis
➢ reduction of estimation uncertainties (combined evaluation, “super fit”) ➢ detect and resolve data inconsistencies (reliable/consistent diagnostics)
➢ resolve parametric entanglement ➢ resolve complex error propagation (non-Gaussian) ➢ synergistic effects (parametric correlations, multi-tasking tools (TS/IF, CXRS/BES)) ➢ automatic in-situ and in-vivo calibration (transient effects, degradation, ...)
➢ replace combination of results from individual diagnostics ➢ with combination of measured data → one-step analysis of pooled data ➢ in a probabilistic framework (unified error analysis!)
Thomson Scattering data analysis ne(x),Te(x) ECE data analysis Te(x) mapping ρ(x) mapping ρ(x) linked result ne(ρ), Te(ρ), ... mapping ρ(x) → ne(x), Te(x) DTS(ne(x)),Te(x)) Thomson Scattering data dTS DECE(ne(x)),Te(x)) ECE data dECE result: p(ne(ρ),Te(ρ) | dTS,dECE) addl. information, constraints, model params, ...
conventional IDA (Bayesian probability theory)
estimates: ne(ρ) ± Δne(ρ), Te(ρ) ± ΔTe(ρ)
Parametric entanglements
(cumbersome; do they exist?)
(Single estimates as input for analysis of other diagnostics?)
(How to deal with inconsistencies?)
(huge amount of data from steady state devices: W7X, ITER, ...)
(sufficient? non-linear dependencies?)
Drawbacks of conventional data analysis: iterative Probabilistic combination of different diagnostics (IDA)
✔ uses only forward modeling
(complete set of parameters → modeling of measured data)
✔ additional physical information easily to be integrated ✔ systematic effects → nuisance parameters ✔ unified error interpretation → Bayesian Probability Theory ✔ result: probability distribution of parameters of interest
IDA offers a unified way
to obtain improved results
Reasoning about parameter θ: (uncertain) prior information + (uncertain) measured data + physical model + Bayes theorem + additional (nuisance) parameter β + parameter averaging (model comparison) p∣d = pd∣× p pd
p likelihood distribution prior distribution d=D D= f pd∣ posterior distribution p∣d =∫ d p ,∣d marginalization (integration) generalization of Gaussian error propagation laws =∫ d pd∣ ,× p× p pd prior predictive value pd∣M =∫d p , d∣M =∫ d pd∣ , M p
Reasoning about parameter ne, Te: (uncertain) prior information + experiment 1: + experiment 2: + experiment 3: + experiment 4: + Bayes theorem pne ,T e∣d TS ,d ECE , d LiB ,d DCN ∝ pd TS∣ne ,T e × pne ,T e likelihood distributions prior distribution dTS=DTSne ,T e ; pd TS∣ne ,T e posterior distribution d ECE=DECET e ; pd ECE∣T e d LiB=DLiBne ,T e ; pd LiB∣ne ,T e d DCN=D DCN ne ; pd DCN∣ne pd ECE∣T e × pd LiB∣ne ,T e × pd DCN∣ne × pne ,T e
Plasma Phys. Control. Fusion, 45, 1095-1111 (2003)
W7-AS: ne, Te: Thomson scattering, interferometry, soft X-ray Electron density 30% reduced error Using synergism: Combination of results from a set of diagnostics
→ synergism by exploiting full probabilistic correlation structure
⊗
Thomson Scattering Soft-X-ray
e
dT
JET: ne , Te : Interferometry, core LIDAR and edge LIDAR diagnostics ne : Lithium beam forward modelling
at JET, P-2.148, EPS 2009, Sofia O Ford, et al., Bayesian Combined Analysis of JET LIDAR, Edge LIDAR and Interferometry Diagnostics, P-2.150, EPS 2009, Sofia
82, 073503 (2011)
TJ-II: ne : Interferometry, reflectometry, Thomson scattering, and Helium beam
Full forward model for Interferometry Reflectometry (group delay) Partial forward model for Thomson scattering Helium beam
➢ Lithium beam impact excitation spectroscopy ➢ Interferometry measurements (DCN) ➢ Electron cyclotron emission (ECE) ➢ Thomson scattering (TS) ➢ Reflectometry (REF) ➢ Equilibrium reconstructions for diagnostics mapping (LiB) (1) ne , Te : (2) Zeff : ➢ Bremsstrahlung background from various CXRS spectroscopies ➢ Impurity concentrations from CXRS
Upgrade, Fusion Sci. Technol., 58, 675-684 (2010)
ASDEX Upgrade with Integrated Data Analysis, PPCF, 52, 095008 (2010)
LIN: Lithium beam only IDA: Lithium beam + DCN Interferometry
#22561, 2.045-2.048 s, H-mode, type I ELM
density profiles with temporal resolution of
➔ simultaneous: ✔ full density profiles ✔ (partly) temperature profiles ➔
→ pressure profile
➔ ne > 0.95*ne,cut-off → masking of ECE channels ➔ opt. depth ~ neTe → masking of ECE channels
✔ forward modeling only (synthetic diagnostic) ✔ probability distributions: describes all kind of uncertainties ✔ multiply probability distributions, marginalization of nuisance parameters ✔ parameter estimates and uncertainties
➢ Probabilistic modeling of individual diagnostics ➢ Probabilistic combination of different diagnostics
✔ systematic and unified error analysis is a must for comparison of diagnostics ✔ error propagation beyond single diagnostics ✔ more reliable results by larger (meta-) data set (interdependencies, synergism) ✔ redundant information → resolve data inconsistencies ✔ advanced data analysis technique → software/hardware upgrades
➢ Applications at W7-AS, JET, TJ-II, and ASDEX Upgrade