A maximum likelihood analysis of the L-H transition DB Darren McDonald 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 1/13 Introduction • • Is L-H scaling sensitive to error models + if so, is the appropriate one used? OLS fits are appropriate when 1. Errors in P >> than in other parameters 2. Relative errors same for all experiments 3. Logs of variables ≈ Normally distributed • • All are violated to some extent Use Maximum-Likelihood to test impact 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 2/13 Maximum-Likelihood method • Soln is one which makes data most likely c c c P f x ; c c S B n • For Likelihood is 1 3 2 I 1 pP | x, c eff ,i exp 12 2 i 1 I Pi f (x i ; c) i 1 eff ,i 2 2 2 4 eff ,i 2 p ,i 2 2 f (x i ; c) i, j 2 x j 1 i, j J • Problem is now Non-Linear, but has been solved by MINUIT package. Take IAE04R dataset. 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 3/13 OLS model - assumptions 1. Errors in P >> than in other parameter 2. Relative errors same for all experiments 3. Logs of variables ≈ Normally distributed 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 4/13 OLS model - fits • M-L model + i), ii) and iii) agrees with OLS • Now relax assumptions in turn Statistical model c1.102 cS cB cn 1. OLS 7.7 0.80 0.65 0.44 2. M-L with i), ii) and iii) 7.7 0.80 0.65 0.44 3. EVOR 7.5 0.85 0.58 0.56 mean 7.5 0.85 0.58 0.56 5. M-L with ii) and iii) only 7.5 0.85 0.58 0.56 6. M-L with iii) only 7.7 0.97 0.32 0.88 7. OLS adjusted for log bias 7.6 0.80 0.65 0.44 4. EVOR with errors 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 5/13 EVOR model - assumptions 1. Errors in P >> than in other parameter • Relax to include all errors 2. Relative errors same for all experiments 3. Logs of variables ≈ Normally distributed 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 6/13 EVOR model - fits • M-L model + ii) and iii) agrees with EVOR • Two methods for averaging errors ≈ same answer • Differ from OLS OLS biases result Statistical model c1.102 cS cB cn 1. OLS 7.7 0.80 0.65 0.44 2. M-L with i), ii) and iii) 7.7 0.80 0.65 0.44 3. EVOR 7.5 0.85 0.58 0.56 mean 7.5 0.85 0.58 0.56 5. M-L with ii) and iii) only 7.5 0.85 0.58 0.56 6. M-L with iii) only 7.7 0.97 0.32 0.88 7. OLS adjusted for log bias 7.6 0.80 0.65 0.44 4. EVOR errors with 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 7/13 Log M-L model - assumptions 1. Errors in P >> than in other parameter • Relax to include all errors 2. Relative errors same for all experiments • Relax to allow machine-machine variation 3. Logs of variables ≈ Normally distributed 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 8/13 Log M-L model - fits • M-L model iii) only differs from OLS and EVOR assumption ii) biases results • Are we sure about tokamak error estimates? • Easy to extend to point-point variation Statistical model c1.102 cS cB cn 1. OLS 7.7 0.80 0.65 0.44 2. M-L with i), ii) and iii) 7.7 0.80 0.65 0.44 3. EVOR 7.5 0.85 0.58 0.56 mean 7.5 0.85 0.58 0.56 5. M-L with ii) and iii) only 7.5 0.85 0.58 0.56 6. M-L with iii) only 7.7 0.97 0.32 0.88 7. OLS adjusted for log bias 7.6 0.80 0.65 0.44 4. EVOR errors with 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 9/13 M-L model - assumptions 1. Errors in P >> than in other parameter • Relax to include all errors 2. Relative errors same for all experiments • Relax to allow machine-machine variation 3. Logs of variables ≈ Normally distributed • Relax by using real variables 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 10/13 M-L model - fits • M-L model differs again skewing of logs influences results • Attempt to correct this in OLS method (7) failed • Are we sure real errors are Normally distributed? Statistical model c1.102 cS cB cn 1. OLS 7.7 0.80 0.65 0.44 2. M-L with i), ii) and iii) 7.7 0.80 0.65 0.44 3. EVOR 7.5 0.85 0.58 0.56 mean 7.5 0.85 0.58 0.56 5. M-L with ii) and iii) only 7.5 0.85 0.58 0.56 6. M-L with iii) only 7.7 0.97 0.32 0.88 7. OLS adjusted for log bias 7.6 0.80 0.65 0.44 8. M-L,Errors on P only 5.6 0.86 0.72 0.58 9. M-L 6.0 0.96 0.45 0.80 4. EVOR with errors 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 11/13 Consistency, errors and ITER Statistical model c1.102 cS cB cn χ2N PITER OLS 7.7 ± 0.3 0.80 ± 0.01 0.65 ± 0.03 0.44 ± 0.03 7.43 35.6 EVOR 7.5 ± 0.3 0.85 ± 0.02 0.58 ± 0.03 0.56 ± 0.03 7.09 43.4 M-L 6.0 ± 0.3 0.96 ± 0.02 0.45 ± 0.04 0.80 ± 0.05 6.26 59.0 • All models differ by more than their errors • M-L gives lowest χ2N for model, but still >>1 model still has missing features must improve before confidence can be placed in this method • ITER prediction highest for M-L 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 12/13 Conclusion • M-L method shown consistent with OLS and EVOR where assumptions are the same • All three assumptions looked at biased scaling • χ2N >> 1 model has missing features must have refine error model to use method • ITER prediction higher for M-L • Prudent estimates may come from average of a set of error models 9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 13/13
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