The Concept of Integrated Data Analysis
- f Complementary Experiments
- R. Fischer,
, A. Din inklag age
Max-Planck-Institut für Plasmaphysik, Garching & Greifswald EURATOM Association Saratoga Springs, July 8-13, 2007
MaxEnt 2007
The Concept of Integrated Data Analysis of Complementary Experiments - - PowerPoint PPT Presentation
MaxEnt 2007 The Concept of Integrated Data Analysis of Complementary Experiments R. Fischer, , A. Din inklag age Max-Planck-Institut fr Plasmaphysik, Garching & Greifswald EURATOM Association Saratoga Springs, July 8-13, 2007
MaxEnt 2007
is a major step in the analysis of experimental data from nuclear fusion devices
combination of measured data → one-step analysis of pooled data
Outliers, inconsistent data, signal-background separation
Challeng nges for data anal alysis is for fus usion
Reliable diagnostics
(data consistency)
⇒ Systematic and unified error analysis
ll sta tatistic ical and systematic errors
ment when we ta talk about t “error”, , “uncerta tainty ty”, “reli liabili lity”, , “signif ific icance”, “evidence”, …
Parameter correlations
(e.g. TS: Te correlated with ne)
⇒ non-Gaussian distributions in data and p parameters
tion? → generaliz izati tion of Gaussia ian error prop.
⇒ Robust estimation
modelin ing
mapping, equilibrium calc., transport calc. ⇒ Combination with modeling Profiles and Gradients ⇒ nonparametric function estimation
flexible le AND reli liable
... an and we want to combi bine/ e/link nk di diagn gnostics ⇒ Validate theoretical models Model complexity ⇒ Model comparison
.g. number of spectral l lines
Multi-tasking tools
(e.g. CXRS/BES or TS/IF)
⇒ Analysis of SETS of diagnostics for synergistic effects
(complementary diagnostics)
Transient effects
(e.g. W/Be/C deposit ition/erosio ion on mirrors, , degradati tion of glas fi fibers, etc.)
⇒ Combination of data for automatic in-situ calibration Combined evaluation
(“super fit”: TS, ECE, LiB, etc.)
⇒ Error reduction by combination of diagnostics
(combination of f data ta NOT result lts)
Diagnostics interdependencies
(e.g. TS, Zeff, CXRS, BES, etc.)
⇒ “One-step” analysis by combination of diagnostics
(complex error propagation!) !)
Consistent diagnostics
(global data consis istency)
⇒ Exploit redundant information
(provide in informatio ion to resolv lve data in inconsistencies)
... comb mbin ine/li link dia iagnostic ics:
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) 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, ...
con
ention
IDA (Bayesian proba bability theo eory)
estimates: ne(ρ) ± Δne(ρ), Te(ρ) ± ΔTe(ρ)
1) 1) 1) 1) Bayesian Modell lling Bayesian Modell lling
⇒ Physical model: quantity of interest ↔ data ⇒ Statistical model: IDA requires a system ematic and formaliz ized error analysis of all uncertaintie ies involved in each diag agnostic to allow for a comparable and relia iable le error analy lysis of different diagnostics. An elaborate error analysis is a MUST for the next step! 2) 2) 2) 2) Bayesian Integration: Li Linkage of Diagnostics Models ls Bayesian Integration: Li Linkage of Diagnostics Models ls ⇒ Combine statistical models of individual diagnostics ⇒ Additional information (physical constraints, modeling, ...) (identification a and quantification of errors: e extensive workload for diagnostician)
quantify with probability distributions (pdf)
ta, , .. ...) .) → likelihood pdf
transmis issivity ty, mir irror reflectiv ivity, , .. ...) .)
→ pdf on hyperparameter
, ...) .) → pdf on model parameter
asma ma equilib ibri rium calc lc., ., etc tc)
(systematic effects, uncerta tain model parameter, , etc.) .)
Generalization of Gaussian error propagation laws
Set of data {d_i} (from subsequent measurements or different
t dia iagnostics) → parameter Θ
One-step analysis:
p∣ d∝∏i pd i∣ p
Bayesian theorem Sequential analysis:
p∣d1∝ pd1∣ p
posterior using first data
p∣d1,d 2∝ pd 2∣d1, p∣d1
use old posterior as new prior
p∣ d∝ pd N∣d N −1 ,,d1, pd 2∣d1,× pd1∣× p ⋮
product rule For independent data:
p∣ d∝ pd N∣ pd 2∣× pd1∣× p ∝∏i pd i∣ p
Sequential ≡ one-step data analysis! Provided we use full probability distributions!
⊗ ⊗ =
Thomson Scattering Soft-X-ray Interferometer Operation Int ntegrated Result
A. . Dinkl klage, E. Pasch, P PPCF 2 2002, PPCF 2003
Electron density 30% reduced error
⊗
Thomson Scattering Soft-X-ray
e
dT
nonparametric function estimation → flexible profile reconstruction hybrid
id: polygon ↔ exp. spline ↔ splin ine
→ smooth and rapid function changes → integration over spline knot amplitudes and positions, number of knots, and
→ robust gradient reconstruction more fl
flexible le than parametric functio ion estima mati tion (tanh)
less fl
flexible le than pointw twis ise reconstructi tion (opti timal knot t numbers)
reduced curvatu
ture regula lariz izati tion
→ uncertainties on profile gradients
W7-AS #54285
AIP 2005
Fischer et a al., to be published
✔ probability distributions: describes all kind of uncertainties ✔ multiply probability distributions, marginalization of nuisance parameters ✔ generalization of Gaussian error propagation
➢ Probabilistic modeling of individual diagnostics ➢ Probabilistic combination of different diagnostics ➢ Topics
✔ 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 → provide information to resolve data inconsistencies ✔ robustness in a harsh environment ✔ flexibility vs. reliability: profile and profile gradients, model comparison ✔ robust estimation (outliers, inconsistent data, signal – background separation) ✔ IDA and Bayesian Experimental Design