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1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph + , Tirthankar Dasgupta* and C. F. Jeff Wu + + ISyE, Georgia Tech *Statistics, Harvard

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Page 1: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED)

V. Roshan Joseph+, Tirthankar Dasgupta* and C. F. Jeff Wu+

+ ISyE, Georgia Tech

*Statistics, Harvard

Page 2: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Statistical modeling and analysis for robust synthesis of nanostructures

Dasgupta, Ma, Joseph, Wang and Wu (2008), Journal of The American Statistical Association, to appear.

Robust conditions for synthesis of Cadmium Selenide (CdSe) nanostructures derived New sequential algorithm for fitting

multinomial logit models. Internal noise factors considered.

Fig 4: CdSe nanostructuresFig 4: CdSe nanostructures

Page 3: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Fitted quadratic response surfaces & optimal conditions

Page 4: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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The need for more efficient experimentation

A 9x5 full factorial experiment was too expensive and time consuming.

Quadratic response surface did not capture nanowire growth satisfactorily (Generalized R2 was 50% for CdSe nanowire sub-model).

Page 5: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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What makes exploration of optimum difficult?

Complete disappearance of morphology in certain regions leading to large, disconnected, non-convex yield regions.

Multiple optima.

Expensive and time-consuming experimentation 36 hours for each run Gold catalyst required

Page 6: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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“Actual” contour plot of CdSe nanowire yield Obtained by averaging yields

over different substrates.

Large no-yield (deep green region).

Small no-yield region embedded within yield regions.

Scattered regions of highest yield.

Page 7: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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How many trials needed to hit the point of maximum yield ?

Pre

ssur

e

Temperature

Page 8: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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How many trials ? Let’s try one factor at-a-time !

Temperature

Pre

ssur

e

Could not find optimumAlmost 50% trials wasted (no yield)Too few data for statistical modeling

Page 9: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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A 5x9 full-factorial experiment

Yield = f(temp, pressure)

17 out of 45 trials wasted (no morphology)!

Pre

ssur

e

Page 10: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Why are traditional methods inappropriate ?

Need a sequential approach to keep run size to a minimum.

Fractional factorials / orthogonal arrays Large number of runs as number of levels increase. Several no-morphology scenarios possible. Do not facilitate sequential experimentation.

Response Surface Methods Complexity of response surface. Categorical (binary in the extreme case) possible.

Page 11: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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The Objective

To find a design strategy that

Is model-independent, Can “carve out’’ regions of no-morphology

quickly, Allows for exploration of complex response

surfaces, Facilitates sequential experimentation.

Page 12: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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What if design points are positively charged particles ?

q1

q2

E = Kq1q2 / d

Charge inversely proportional to yield,e.g., q = 1-yield

Pre

ssur

e

= 0.6

= 1.0

Y = 40%

Y = 0

Page 13: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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What position will a newly introduced particle occupy ?

q1

q2

Pre

ssur

e

= 0.6

= 1.0

Total Potential E

nergy Minimized !!

Page 14: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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The key idea

Pick a point x. Conduct experiment at x and observe yield y(x). Assign charge q(x) inversely proportional to y(x)

How quickly will you reach the optimum ? Once you reach there, how will you know that THIS IS IT ?

Use y(x) to update your knowledge about yields at various points in the design space (How ?)

Pick the next point as the one that minimizes the total potential energy in the design space.

Page 15: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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The SMED algorithm

Page 16: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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The next design point

Page 17: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Charge at unselected points

Page 18: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Choice of tuning constants

PROPOSITION : There exists a value of (inverse of the maximum yield pg) for which the algorithm will stick to the global optimum, once it reaches there.

In practice, pg will not be known. The constant determines the rate of

convergence. Both and will be estimated iteratively.

Page 19: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Performance with known

Page 20: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Performance with known (Contd.)

Page 21: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Performance with known (Contd.)

Initial point = (0.55,0.50) Initial point = (0.77,0.50)

Page 22: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Criteria for estimators of and

.increases) as local more(Search (ii)

,/1 ,/1 (i)

:tsRequiremen

maximum. Global :

iteration,th the tillyield maximum Observed :

iteration,th after the and of Estimators :,

)(

)(

pp

p

np

n

n

nngn

g

n

nn

Page 23: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Iterative estimation of and

constant a is where,/1

)/1log(

0 where,)1(

1

)()(

na

apap

n

nn

nnnn

n

Page 24: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Improved SMED for random response

Instead of an interpolating function, use a smoothing function to predict yields (and charges) at unobserved points.

Update the charges of selected points as well, using the smoothing function.

Local polynomial smoothing used. Two parameters:

nT (threshold number of iterations after which smoothing is started).

(smoothing constant; small local fitting).

Page 25: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Improvement achieved for r = 5

Last row gives the performance of the standard algorithm. Modified algorithm

significantly improves the number of times the global optimum is reached,

does worse with respect to no-yield points (higher perturbation).

Page 26: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Summary A new sequential space-filling design SMED

proposed. SMED is model independent, can quickly “carve out”

no-morphology regions and allows for exploration of complex surfaces.

Origination from laws of electrostatics. Algorithm for deterministic functions. Modified algorithm for random functions. Performance studied using nanowire data, modified

Branin (2 dimensional) and Levy-Montalvo (4 dimensional) functions.

Page 27: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Predicting the future

What the hell! I don’t want to use this stupid strategy for experimentation !

Use my SMED !

Image courtesy : www.cartoonstock.com

Nano

Stat

Page 28: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Page 29: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Advantages of space filling designs

LHD (McCay et al. 1979), Uniform designs (Fang 2002) are primarily used for computer experiments.

Can be used to explore complex surfaces with small number of runs.

Model free. No problems with categorical/binary data. CAN THEY

BE USED FOR SEQUENTIAL EXPERIMENTATION ? CARVE OUT REGIONS OF NO-MORPHOLOGY QUICKLY?

Page 30: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Sequential experimentation strategies for global optimization

SDO, a grid-search algorithm by Cox and John (1997) Initial space-filling design. Prediction using Gaussian Process Modeling. Lower bounds on predicted values used for sequential selection

of evaluation points. Jones, Schonlau and Welch (1998)

Similar to SDO. Expected Improvement (EI) Criterion used. Balances the need to exploit the approximating surface with the

need to improve the approximation.

Page 31: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Why they are not appropriate Most of them good for multiple optima, but

do not shrink the experimental region fast.

Algorithms that reduce the design space (Henkenjohann et al. 2005) assume connected and convex failure regions.

Initial design may contain several points of no-morphology.

Current scenario focuses less on convergence and more on quickly shrinking the design space.

Page 32: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Some performance measures for n0 - run designs.

Page 33: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Performance with estimated and with 30-run designs

Page 34: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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First 20 iterations (out of 30) with estimated and

Page 35: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Contour plots of estimated p(x) (=y/r) where y ~ binomial(r,p(x))

Page 36: 1 Efficient experimentation for nanostructure synthesis using Sequential Minimum Energy Designs (SMED) V. Roshan Joseph +, Tirthankar Dasgupta* and C

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Performance of the algorithm with random response

Result of 100 simulations with = 1.25, starting point = (0,0).

The last row represents the case of deterministic response and first three random response.

Concern: as r decreases, the number of cases in which the global optimum is identified reduces drastically.