65
!"#$"#% # !"#$%&' ) *+,- # !"#$% '()*+% ,-./)*.-0) 1/)23*4.24/% 5( 36) 7($8%3-2$8 '8)23*4( 9-2*4.24/) :).34* ;< =$8>?)2 ?$8>?)2@A-2*4.24/%<24A ?$8>?)2@$$)A<$A2<$(8<+40 !"#$%&' ) *+,- & ./&'0123'2/4 567"#408'"# 9"/":8#808&3 440 460 480 500 520 540 560 Energy Loss (eV) XEDS EELS 20 18 16 14 12 10 8 6 4 2 0 0 1000 2000 3000 4000 En erg y (k eV) &'()

Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 1: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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XEDS

EELS

2 01 81 61 41 21 0864200

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2 0 0 0

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4 0 0 0

Energ y (keV)

&'()

Page 2: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 3: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Energy Loss (eV)

BBD.

20181614121086420 101086Energy (keV)

EB=.-(./(01.2

-(./(01.2

400 500 600 700 800 900 1000Energy (eV)

34 51 6

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Page 4: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 5: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Nomenclature for Principle X-ray Emission Lines

N Shell

H6$*$23)*-.3-2& !"*$%& F-()&'()*+%&&&&K&&&'&G-($8&" '&-(-3-$8

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Page 6: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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1>/)*24(E>23-(+& H$84*-A)3)*.]^484A)3)*.

Page 7: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 8: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 9: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

!"#$"#%

%

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0

10

20

30

40

50

60

70

0 50 100 150 200 250

Comparing SDD vs Si(Li) @ Eo = 300 keV

Dea

d Ti

me

(%)

Input Count Rate (Kcps)

1-NF-P 1,,

=&"I(a8<&(P3(92$70(A"0&

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Si(Li) vs SDD

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SDD - 1.0 mm

Si(Li) - 3.0 mm

Rel

ativ

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Energy (eV)

d/98.1Z/<@/./D.KJ< >TT1D1/(D2<

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Page 10: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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WindowlessXEDS Detector

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Energy (keV)

O K

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Detector/Specimen Geometry

7K(.1(HH)<^1SR92<P(10K.JKC1D

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! =SR2 "

AR2

Page 11: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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CM200 Normalized vs Energy (keV)CM30 Normalized vs Energy (keV)Tecnai Normalized vs Energy (keV)

0

1000

2000

3000

4000

5000

6000

7000

8000

9000

10000

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12000

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7.2 7.3 7.4 7.5 7.6 7.7 7.8

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IK!Ni!

Page 12: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Variation in Collection Solid Anglewith Specimen to Detector Crystal Distance

100 mm^250 mm^230 mm^210 mm^2

Col

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Sol

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2!

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d

A

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Page 13: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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1.4 1.5 1.6 1.7 1.8 1.9 2.0 2.1 2.2

Page 14: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 15: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 16: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 17: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Page 18: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Nanochemistry of Phases in Obsidian (MMF is Important here)

200 nm

Log

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O

Na

Al

Cl

Si

KCa

Fe

Ti

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Element Z 10nm 50nm 100nm 500nm50nm 100nm 500nmElementElementCarbon

ZZ6

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500nm500nm57.4Carbon

Aluminium 613

0.160.26

1.81.9

5.138.12

57.490.9Aluminium Aluminium

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0.260.260.68

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Spatial Resolution /Beam Spreading Monte Carlo Calculations

DC Joy's MC Program

Al

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Monte Carlo Calculations of Monte Carlo Calculations of BB (Newbury & Myklebust (Newbury & Myklebust -(Newbury & Myklebust -1979)Monte Carlo Calculations of Monte Carlo Calculations of B (Newbury & Myklebust (Newbury & Myklebust (Newbury & Myklebust (Newbury & Myklebust (Newbury & Myklebust 1979)1979)1979)

ThicknessElement Z 10nm

Thickness50nmThickness

100nm 500nmElement Z 10nm 50nm 100nm100nm 500nm

Carbon 6 0.22 1.9 4.1 33.0Carbon Aluminium

613

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1.93.0

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3.05.8

7.617.5

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Data Analysis and Quantification

Spectral ProcessingThin Film Quantification MethodsSpecimen Thickness Effects:

AbsorptionFluorescence

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Spectrum = Characteristic Peaks + Background

Data Reduction

Simple: Linear Background Fit & Integration

Curve Fitting: Non-Linear Background & Profile Matching

Frequency (Digital) Filtering: Background Suppression& Reference Spectra Fitting

Deconvolution: Fourier Method for Resolution Enhancement

Background Modeling

Simple - Linear and/or Polynominal Interpolation

Modeling - Parametric Fits of Analytic ExpressionsPhenomenological ExpressionsModified Bethe Heitler ModelDigital Filtering - Mathematical Supression

a*

Page 30: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Spectral Processing : XEDSSimple Data Reduction

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Page 31: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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Background Modeling : Power Law/Parametric Fits

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Spectral Processing : XEDS

Background Modeling : Power Law/Parametric Fits

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Quantitative Analysis Equations

For a thin specimen

IIA = Measured xMeasured x-Measured x-ray intensity Measured xMeasured xMeasured x-ray intensity ray intensity ray intensity per unit area

- = KKthKthKthK -per unit areaper unit areaper unit areaper unit areaper unit areaper unit area

th-shell ionization crossshell ionization cross-shell ionization crossshell ionization cross-section-.

==

KKKKKthKKKththKthK -

shell ionization crossshell ionization crossshell ionization crossshell ionization crossshell ionization crossshell ionization cross-sectionsectionsectionshell ionization crossshell ionization cross-shell ionization crossshell ionization crossshell ionization crossthth shell fluorescence yield..

/===

KKKKKKKthKthKthKKKKththKthK -

shell fluorescence yieldshell fluorescence yieldshell fluorescence yieldshell fluorescence yieldshell fluorescence yieldshell fluorescence yieldshell fluorescence yieldshell fluorescence yieldth-shell fluorescence yieldshell fluorescence yieldshell fluorescence yield-shell fluorescence yieldshell fluorescence yieldthth-shell radiative partition function//

W==

KKKKKK -shell radiative partition functionshell radiative partition functionshell radiative partition functionshell radiative partition functionshell radiative partition functionshell radiative partition functionshell radiative partition functionshell radiative partition functionAtomic WeightWW

NNo

===

Atomic WeightAtomic WeightAtomic WeightAtomic WeightAtomic WeightAtomic WeightAvagodro's numberNNNNooNoNNoN

(===

Avagodro's numberAvagodro's numberDensity((

C==

DensityDensityComposition (At %)CC

%%o

===

Composition (At %)Composition (At %)Incident electron flux%%%oo

t===

Incident electron fluxIncident electron fluxSpecimen thicknesstt

'= = =

Specimen thicknessSpecimen thicknessDetector efficiency''

0===

Detector efficiencyDetector efficiencyDetector solid angle

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vsTheory

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Variation in Measured Composition on 308 SS for Different Labs

Example in which KExample in which K-Example in which K-Example in which K-Example in which K factor is stable Example in which KExample in which KExample in which K-Example in which K-Example in which K factor is stable factor is stable factor is stable Cr, Fe, Ni Cr, Fe, Ni Cr, Fe, Ni Cr, Fe, Ni Cr, Fe, Ni

Note: Detector efficiency ~ 100% in this energy range

Page 35: Zaluzec-XEDS-20190616-Uppsala - teknik.uu.se · i-. / (% '!"#$%&'()*+,-!! ^]'^&!"#$"#% *+!"#$%&'()*+,-!$

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From: Comparison of UTW/WL XFrom: Comparison of UTW/WL X-From: Comparison of UTW/WL X-ray Detectors on TEM/STEMs and STEMs

Thomas, Charlot, Franti, GarrattThomas, Charlot, Franti, Garratt-Thomas, Charlot, Franti, Garratt-Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Thomas, Charlot, Franti, GarrattThomas, Charlot, Franti, GarrattThomas, Charlot, Franti, Garratt-Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Analytical Electron Microscopy

Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Analytical Electron MicroscopyAnalytical Electron Microscopy-

Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Reed, Goodhew, Joy, Lee, Ng, Plicta, Zaluzec.Analytical Electron MicroscopyAnalytical Electron Microscopy-1984 1 09876543210

0.0

0.2

0.4

0.6

0.8

1.0

X-ray Photon Energy (keV)

Calc

ulat

ed

Det

ecto

r Ef

fici

ency

S i ( L i )

HP GeDetector Parameters

Be Window: 0 nmGold Contact: 20 nmSi Dead Layer: 100 nmSi Active Layer: 3 mmGe Dead Layer: 200 nmGe Active Layer: 3 mm

20

30

40

50

60

70

80

0 1 2 3 4 5 6 7 8

NiO

Co

mp

osi

tio

n (

At

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Lab

513

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Sources of values for kSources of values for kAB AB AB CalculationsSources of values for kSources of values for kAB Sources of values for kAB CalculationsCalculationsAB Calculations

W -- International Tables of Atomic Weights

//(K) -- Schreiber and Wims , XSchreiber and Wims , X-Schreiber and Wims , X-ray Spectroscopy (1982)Schreiber and Wims , XSchreiber and Wims , XSchreiber and Wims , X ray Spectroscopy (1982)ray Spectroscopy (1982)ray Spectroscopy (1982)Vol 11, p. 42

//(L) -- Scofield, Atomic and Nuclear Data Tables (1974)Scofield, Atomic and Nuclear Data Tables (1974)Vol 14, #2, p. 121

.. (K) (K) -- Bambynek etal, Rev. Mod. Physics, Vol 44, p. 716Bambynek etal, Rev. Mod. Physics, Vol 44, p. 716Freund, X

Bambynek etal, Rev. Mod. Physics, Vol 44, p. 716Freund, XFreund, X-

Bambynek etal, Rev. Mod. Physics, Vol 44, p. 716Bambynek etal, Rev. Mod. Physics, Vol 44, p. 716Bambynek etal, Rev. Mod. Physics, Vol 44, p. 716Freund, XFreund, X-ray Spectrometry, (1975) Vol 4, p.90

..(L) -- Krause, J. Phys. Chem. Ref. Data (1974) Vol 8, Krause, J. Phys. Chem. Ref. Data (1974) Vol 8, p.307

--(Eo) -- Inokuti, Rev. Mod. Physics, Inokuti, Rev. Mod. Physics, 4343, 4343 No. 3, 297 (1971)Inokuti, Rev. Mod. Physics, -

Inokuti, Rev. Mod. Physics, Inokuti, Rev. Mod. Physics, 4343Inokuti, Rev. Mod. Physics, 4343Inokuti, Rev. Mod. Physics, - Goldstein etal, SEM

43434343Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM 1

No. 3, 297 (1971)No. 3, 297 (1971)No. 3, 297 (1971)43, No. 3, 297 (1971)No. 3, 297 (1971)43, 11, 315, (1977)

-Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM

- Chapman etal, XGoldstein etal, SEM Goldstein etal, SEM Chapman etal, X-Goldstein etal, SEM Goldstein etal, SEM , 315, (1977) , 315, (1977) , 315, (1977) , 315, (1977) , 315, (1977) 1, 315, (1977) , 315, (1977) , 315, (1977) Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Goldstein etal, SEM Chapman etal, X-ray Spectrometry, ray Spectrometry, 121212,153,(1983)

-Chapman etal, XChapman etal, XChapman etal, XChapman etal, X

- Rez, XChapman etal, XChapman etal, XRez, X-Chapman etal, XChapman etal, XChapman etal, XChapman etal, XChapman etal, XChapman etal, X ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, Chapman etal, XChapman etal, XChapman etal, XChapman etal, XRez, X-ray Spectrometry,

ray Spectrometry, ray Spectrometry, ray Spectrometry, 13

ray Spectrometry, ray Spectrometry, 13,

ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, 12121212,153,(1983),153,(1983)121212,153,(1983)ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, 13, 55, (1984)

-Rez, XRez, XRez, XRez, XRez, XRez, X ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, ray Spectrometry, Rez, XRez, X

- Egerton, Ultramicroscopy, 1313

Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, 455, (1984)55, (1984)55, (1984)55, (1984)55, (1984)55, (1984)55, (1984)55, (1984)55, (1984)55, (1984)55, (1984)1313, ,

4444, 169, (1969)-

Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, - Zaluzec, AEM

Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Zaluzec, AEMZaluzec, AEM-Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, 44, 169, (1969), 169, (1969), 169, (1969), 169, (1969), 169, (1969), 169, (1969), 169, (1969)4, 169, (1969)Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Egerton, Ultramicroscopy, Zaluzec, AEMZaluzec, AEM-1984, San Fran. Press. 279, (1984)

'' (E) -- Use mass absorption coefficients from:Use mass absorption coefficients from:-

Use mass absorption coefficients from:Use mass absorption coefficients from:-Thinh and Leroux; X

Use mass absorption coefficients from:Thinh and Leroux; X-

Use mass absorption coefficients from:Use mass absorption coefficients from:Use mass absorption coefficients from:Thinh and Leroux; X-ray Spect. (1979), ray Spect. (1979), 8,8, p. 963

-Thinh and Leroux; XThinh and Leroux; XThinh and Leroux; XThinh and Leroux; XThinh and Leroux; XThinh and Leroux; X ray Spect. (1979), ray Spect. (1979), ray Spect. (1979), ray Spect. (1979), ray Spect. (1979), ray Spect. (1979), Thinh and Leroux; XThinh and Leroux; X

-Henke and Ebsiu, Adv. in Xray Spect. (1979), ray Spect. (1979),

Henke and Ebsiu, Adv. in X-ray Spect. (1979), ray Spect. (1979), ray Spect. (1979), ray Spect. (1979), ray Spect. (1979), ray Spect. (1979),

Henke and Ebsiu, Adv. in X-ray Analysis,ray Spect. (1979), 8,8, p. 963

ray Analysis,ray Analysis,ray Analysis,ray Analysis,17,p. 963p. 963p. 963p. 963

17,17, (1974)-Henke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in X

-Holton and Zaluzec, AEMHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHolton and Zaluzec, AEMHolton and Zaluzec, AEM-

ray Analysis,ray Analysis,ray Analysis,ray Analysis,ray Analysis,ray Analysis,ray Analysis,ray Analysis,ray Analysis,ray Analysis,17,17,17,17, (1974)(1974)(1974)(1974)ray Analysis,ray Analysis,17,17,17, (1974)ray Analysis,ray Analysis,Henke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHenke and Ebsiu, Adv. in XHolton and Zaluzec, AEMHolton and Zaluzec, AEM--1984, San Fran Press,353,(1984)

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Quantitative Analysis using XEDSStandards based Method

Invoke the Intensity Ratio Method, that is consider the ratio of x-ray lines from the same element in both the Unknown and a Standard

This simple equation states that the relative intensity ratio of the samecharacteristic x-ray lines is directly proportional to the relativecomposition ratio of the elemental components mult iplied by aproportionality factor which, in the thin film approximation, isdependent upon , (, t and %

NOTE: The factor also is not a universal constant, and requires an accurate measurement/determination of density, thickness and beam current.

IAUnknown

IAS tandard =

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=#SU CA

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! t =IA

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! A (E, Z )!A!A( ) CANo( ) not( ) !A"( )=!A

IAK!

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Rearrange the Intensity Equation

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Recognize

!A =WA

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1 098765432100.0

0.2

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X-ray Photon Energy (keV)

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ecto

r Ef

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S i ( L i )

HP GeDetector Parameters

Be Window: 0 nmGold Contact: 20 nmSi Dead Layer: 100 nmSi Active Layer: 3 mmGe Dead Layer: 200 nmGe Active Layer: 3 mm

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Quantitative Analysis using XEDSQuantitative Analysis using XEDSSpecimen Thickness Effects

For finite thickness specimens, what is a thin film?

The Thin Film ApproximationThe Thin Film ApproximationNo Energy lossNo Energy lossNo Energy lossNo XNo Energy lossNo Energy lossNo X-No Energy lossNo Energy lossNo Energy lossNo Energy lossNo Energy lossNo Energy lossNo X ray absorption, No XNo XNo XNo XNo XNo X-

ray absorption, ray absorption, ray absorption, ray absorption, No XNo X-ray absorption, ray absorption, No X-ray fluorescence

/;# <#=;#<#5;#<#>; 3$#?@AB

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Specimen HomogenityInIn thisthis andand allallall otherother derivationsderivations wewewe havehave assumedassumed thatthat overover thethe excitedexcited volume,volume, asasas wellwell as

alongalong thInIn this

thth exitingandandand allallall otherotherthisthis and

exiting pathlength,derivationsotherother

pathlength, thederivationsderivationsderivationsderivations

the specimenderivations we

specimen ishavehavehave assumedassumedwe havewewe

isisis homogeneousassumed that

homogeneous inoveroverover thethethethatthatthatthat

ininin compositionexcitedexcited

compositioncomposition.excitedexcitedexcited

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aswell asassumption isalongalong th

invalid,exitingexitingexitingexitingththth exitingexiting

invalid, oneexitingexitingexitingexiting pathlength,pathlength,exitingexitingone must

pathlength,pathlength,pathlength,pathlength,pathlength,pathlength,pathlength, thethepathlength,pathlength,pathlength,pathlength,pathlength,pathlength,mustmust reformulate

specimenspecimenthethethethethethereformulatereformulate the

specimenspecimenspecimenspecimenspecimen isisisisisisisspecimenspecimenspecimenspecimenthethe absorption

homogeneoushomogeneoushomogeneoushomogeneoushomogeneoushomogeneoushomogeneoushomogeneousabsorptionabsorption correction

homogeneoushomogeneoushomogeneoushomogeneoushomogeneoushomogeneouscorrection and

compositioncompositioncompositioncompositioninininininininand take

compositioncompositioncompositioncompositioncompositioncompositiontake into

compositioncompositioncompositioncompositioncomposition.. IfIfcompositioncompositioncompositioncompositioninto account

thisthisthisthisthisthisthis assumptionassumptionIfIfIfIfaccount changes

assumptionassumptionassumptionassumptionassumptionchangeschangeschanges in

assumptionassumptionassumptionassumptionassumptioninin :

assumptionassumptionassumptionassumptionassumptionassumptionassumptionassumptionassumptionassumption: µ/(, (

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exitingexiting pathlengthabsorptionabsorptionthethethethe absorptionabsorption

pathlengthpathlengthpathlength.

Effects of Beam Broadening

Parallel Slab Model: No Change in absorption pathlengthParallel Slab Model: No Change in absorption pathlengthWedge Model:Parallel Slab Model: No Change in absorption pathlength

There is a correction the magnitude ofThere is a correction the magnitude ofThere is a correction the magnitude ofwhich varies with the wedge angle.

Effects of Irregular Surface

This cannot be analytically modeled but must be understood!

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• Original Observations of Effect Original Observations of Effect –

Original Observations of Effect Original Observations of Effect Duncumb

Original Observations of Effect Original Observations of Effect Duncumb Duncumb

Original Observations of Effect Original Observations of Effect Original Observations of Effect Duncumb Duncumb 62, Hall

Original Observations of Effect Original Observations of Effect 62, Hall 62, Hall

Original Observations of Effect Original Observations of Effect Original Observations of Effect 62, Hall 62, Hall 66, Cherns etal 66, Cherns etal 66, Cherns etal 66, Cherns etal 73

•Duncumb Duncumb Duncumb 62, Hall 62, Hall 62, Hall 62, Hall 62, Hall 66, Cherns etal 66, Cherns etal 66, Cherns etal

Predicted Applications Predicted Applications –

Predicted Applications Predicted Applications Cowley

Predicted Applications Predicted Applications Cowley Cowley

Predicted Applications Predicted Applications Cowley Cowley 64,

Predicted Applications Predicted Applications Predicted Applications Predicted Applications 64, 64, 64, 64,

Predicted Applications Predicted Applications Predicted Applications 64, 64, 70

•Cowley Cowley Cowley 64, 64, 64, 64, 64,

ACHEMI Technique ACHEMI Technique ACHEMI Technique -ACHEMI Technique –

ACHEMI Technique ACHEMI Technique Tafto

ACHEMI Technique ACHEMI Technique Tafto

ACHEMI Technique ACHEMI Technique ACHEMI Technique ACHEMI Technique Tafto 79, Spence & Tafto 79, Spence & Tafto 79, Spence & Tafto 83

• MultiTafto

MultiMulti-79, Spence & Tafto 79, Spence & Tafto 79, Spence & Tafto 79, Spence & Tafto 79, Spence & Tafto 79, Spence & Tafto 838383Tafto Tafto Tafto

MultiMulti-Variate Statistical Analysis Variate Statistical Analysis -–

Variate Statistical Analysis Variate Statistical Analysis Variate Statistical Analysis Variate Statistical Analysis Rossouw etal , Anderson and others Rossouw etal , Anderson and others

late80Rossouw etal , Anderson and others Rossouw etal , Anderson and others

late80late80Rossouw etal , Anderson and others

late80late80 -Rossouw etal , Anderson and others Rossouw etal , Anderson and others

-90Rossouw etal , Anderson and others Rossouw etal , Anderson and others Rossouw etal , Anderson and others Rossouw etal , Anderson and others Rossouw etal , Anderson and others

90909090Rossouw etal , Anderson and others Rossouw etal , Anderson and others Rossouw etal , Anderson and others Rossouw etal , Anderson and others

90909090 s

Electron Channeling Induced XElectron Channeling Induced X-Electron Channeling Induced X-ray Emission

1200

1400

1600

1800

2000

2200

- 2 - 1 0 1 2

AlK

g

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0

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FeKCrKNiK

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AlK-10um NiK-10 um

g

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Orientation Dependance of X-ray EmissionSi K in Amorphous SiO

AlK in Polycrystalline Al

Si*TAl*T

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Orientation (mR)

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