Introduction to Integrated Data Analysis R. Fischer - - PowerPoint PPT Presentation

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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


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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

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Outline

➢ 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

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IDA for Nuclear Fusion

Different measurement techniques (diagnostics: LIB, DCN, ECE, TS, REF, ...) for the same quantities (ne, Te, …) and parametric entanglement in data analysis

  • Redundant data:

➢ reduction of estimation uncertainties (combined evaluation, “super fit”) ➢ detect and resolve data inconsistencies (reliable/consistent diagnostics)

  • Complementary data:

➢ 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, ...)

  • Goal: Coherent combination of measurements from different diagnostics

➢ 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!)

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Conventional vs. Integrated Data 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

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Conventional vs. Integrated Data Analysis (2)

  • (self-)consistent results?

(cumbersome; do they exist?)

  • information propagation?

(Single estimates as input for analysis of other diagnostics?)

  • data and result validation?

(How to deal with inconsistencies?)

  • non-Gaussian error propagation? (frequently neglected: underestimation of the true error?)
  • difficult to be automated

(huge amount of data from steady state devices: W7X, ITER, ...)

  • often backward inversion techniques (noise fitting? numerical stability? loss of information?)
  • result: estimates and error bars

(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

  • f combining data (information) from various experiments (sources)

to obtain improved results

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Probabilistic (Bayesian) Recipe

Reasoning about parameter θ: (uncertain) prior information + (uncertain) measured data + physical model + Bayes theorem + additional (nuisance) parameter β + parameter averaging (model comparison) p∣d = pd∣× p pd 

}

p likelihood distribution prior distribution d=D D= f  pd∣ posterior distribution p∣d =∫ d  p ,∣d marginalization (integration) generalization of Gaussian error propagation laws =∫ d  pd∣ ,× p× p pd prior predictive value pd∣M =∫d  p , d∣M =∫ d  pd∣ , M  p

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Bayesian Recipe for IDA: LIB + DCN + ECE + TS

Reasoning about parameter ne, Te: (uncertain) prior information + experiment 1: + experiment 2: + experiment 3: + experiment 4: + Bayes theorem pne ,T e∣d TS ,d ECE , d LiB ,d DCN ∝ pd TS∣ne ,T e × pne ,T e likelihood distributions prior distribution dTS=DTSne ,T e ; pd TS∣ne ,T e posterior distribution d ECE=DECET e ; pd ECE∣T e d LiB=DLiBne ,T e ; pd LiB∣ne ,T e d DCN=D DCN ne ; pd DCN∣ne pd ECE∣T e × pd LiB∣ne ,T e × pd DCN∣ne × pne ,T e

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Application: W7-AS

  • R. Fischer, A. Dinklage, and E. Pasch, Bayesian modelling of fusion diagnostics,

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

=

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Application: JET

JET: ne , Te : Interferometry, core LIDAR and edge LIDAR diagnostics ne : Lithium beam forward modelling

  • D. Dodt, et al., Electron Density Profiles from the Probabilistic Analysis of the Lithium Beam

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

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Application: TJ-II

  • B. Ph. van Milligen, et al., Integrated data analysis at TJ-II: The density profile, Rev. Sci. Instrum.

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

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Application: ASDEX Upgrade

➢ 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

  • R. Fischer et al., Integrated data analysis of profile diagnostics at ASDEX

Upgrade, Fusion Sci. Technol., 58, 675-684 (2010)

  • S. Rathgeber et al., Estimation of profiles of the effective ion charge at

ASDEX Upgrade with Integrated Data Analysis, PPCF, 52, 095008 (2010)

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LIB + DCN: Temporal resolution

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

  • 1 ms (routinely written)
  • 50 μs (on demand)
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IDA: LIB + DCN + ECE

➔ 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

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Summary: IDA

✔ 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