NSE data reduction - NIST

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NSE tutorial 2-27-2008 How to reduce NSE data to I(Q,t) A. Faraone

Transcript of NSE data reduction - NIST

Page 1: NSE data reduction - NIST

NSE tutorial 2-27-2008

How to reduce NSE data to I(Q,t)

A. Faraone

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Outline• What does NSE measure?

– Polarization vs Phase and Ft.

– How to Eliminate Instrument Dependent Signals.

• How using a 2D detector complicates things?

– How DAVE helps us out.

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Polarized Intensityvs phase and Ft

What do we measure ●○○○○○○○○○

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Polarized Intensity vs phase

What do we measure ●●○○○○○○○○

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Static measurements(Up and Down)

t=0 (J=0): ∫S(Q,ω)dω

I0 Average Intensity

T Period, function of ⟨λ⟩

σ Echo width, function of f(λ) width distribution

ph0 Echo point

A Amplitude, related to I(Q,t)

( ) ( )⎥⎦⎤

⎢⎣⎡ −⎥

⎤⎢⎣

⎡ −+= 02

20

0360cos

2exp phph

TphphAII p

σ

What do we measure ●●●○○○○○○○

Fitting the echo

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The Physical Information is All in the Amplitude

( )( ) DwnUp

AQI

tQI−

∝2,

What do we measure ●●●●○○○○○○

Incidentally, in this way, both polarization and detector efficiency effects are taken care off.

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What do we measure ●●●●●○○○○○

A Small Portion of the Echo will do

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Polarized Intensity vs Ft

What do we measure ●●●●●●○○○○

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Resolution

Even for an elastic scatterer the echo signal will

decrease with the increase of the Fourier time.•Inhomogeneities in the magnetic field will depolarize

the beam.

What do we measure ●●●●●●●○○○

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Resolution Normalization

( )( )RRR DwnUpA

DwnUpAQI

tQI−−

=2

2)0,(),(

What do we measure ●●●●●●●●○○

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Resolution Normalization

In Neutron Spin-Echo the resolution can be

simply divided out from the data.

What do we measure ●●●●●●●●●○

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Blank correction

What do we measure ●●●●●●●●●●

( ) ( ) ( ) ( )( )RRR

BKGBKGBKG

BKGBKG

DwnUpA

DwnUpT

TDwnUpAT

TA

QItQI

⎥⎦⎤

⎢⎣⎡ −−−−⎥⎦

⎤⎢⎣⎡ −−

=2

112

)(),(

φφ

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Take Home Messages• The Physical Information is in the Echo

Amplitude.

• But… You Have to Accurately Fit the Echo to

get the Amplitude right.

• The Resolution can be simply divided out.

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Using a Big DetectorMakes Things Harder

Questions:• What are the advantages of using a 2D detector?

• What are the problems that a 2D detector gives for the

reduction of NSE data?

2D Detector ●○○○○○○○○

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2D Detector

Total Data=32×32×Nphase×NFt≈500000

2D Detector ●●○○○○○○○

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Questions II• What are those thin blue lines?• Does the polarized intensity change with the pixel position? Why?

Up and DownI0ATσ

Ph0

• Yes. Efficiency, Polarization.• Yes.• Yes. Q-dependence.• No.• No.• Yes. Field Integral: ∫Bdl.

2D Detector ●●●○○○○○○

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2D Detector AnalysisThe echoes at each detector pixel have to be fitted individually.

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Binning

2D Detector ●●●●●○○○○

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Phase Map

The Phase Map should be a smoothly varying function of the position on the detector and of the Fourier time.

2D Detector ●●●●●●○○○

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Reducing NSE data with DAVE

1. Mask low intensity areas.

2. Fit the resolution.

3. Make sure the phase map is correct.

4. Remove poor resolution points.

5. Check the χ2.

2D Detector ●●●●●●●○○

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Importing the phase map

The phase map is sample independent. To fit

your sample and background data just…

1. Import the phase map from the resolution.

2. Check the χ2.

2D Detector ●●●●●●●●○

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Calculate I(Q,t)

The Intermediate Scattering function values are

calculated pixel by pixel and averaged,

according to their weight, by Q areas.

( ) ( ) ( ) ( )( )RRR

BKGBKGBKG

BKGBKG

DwnUpA

DwnUpT

TDwnUpAT

TA

QItQI

⎥⎦⎤

⎢⎣⎡ −−−−⎥⎦

⎤⎢⎣⎡ −−

=2

112

)(),(

φφ

2D Detector ●●●●●●●●●

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Conclusion

At the end of the reduction process the I(Q,t)

contains information about your sample only.