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Spectrum Imaging

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... Ni-based superalloy Courtesy M. Watanabe Problems for which MSA may be useful Investigation of data of great complexity Handling large quantities of data ... – PowerPoint PPT presentation

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Title: Spectrum Imaging


1
Spectrum Imaging
Charles Lyman Lehigh University, Bethlehem, PA
Based on presentations by John Hunt (Gatan,
Inc.), John Titchmarsh (Oxford University), and
Masashi Watanabe (Lehigh University)
2
Spectrum Imaging (SI)
  • Collect entire spectrum at each pixel
  • No a priori of specimen knowledge required
  • Can detect small amounts of elements in local
    regions of x-y images
  • Away from microscope
  • Repeatedly apply sophisticated spectrum
    processing
  • Mine the data cube for features
  • Concept
  • Jeanguillaume Colliex, Ultramicroscopy 28
    (1989), 252
  • Demonstration
  • Hunt Williams, Ultramicroscopy 38 (1991), 47

3
Elemental Maps from Data Cube
Elemental X-ray map
X-ray Spectrum
Specimen polished granite
Data courtesy of David Rohde
4
Quantitative Phase Analysis
  • Sum spectra for pixels within box
  • Enough counts for quatitative analysis

Specimen polished granite
Data courtesy of David Rohde
5
Compositional Maps in TEM/STEM
  • Collection by
  • STEM X-ray
  • Sequentially acquire EDS x-ray spectrum at each
    pixel (original concept)
  • Each x-ray entering detector assigned
    x-y-energy tag (Mott Friel, 1999)
  • STEM EELS
  • Sequentially acquire EELS spectrum at each pixel
  • EFTEM (Energy-filtered imaging)
  • Sequentially acquire images at specific energies
  • One energy window for each energy channel in
    spectrum (DE)

6
A few Words about EFTEM Elemental Maps without
Employing Spectrum Imaging
7
EFTEM In-Column and Post-Column Energy Filters
Omega Filter
Gatan Imaging Filter (GIF)
From Williams and Carter, Transmission Electron
Microscopy, Springer, 1996
8
Energy-Filtered TEM (EFTEM) Element Maps - Not
Spectrum Images
Elemental Maps of a SiC/Si3N4 ceramicShort
Acquisition Time (3 maps, 250K pixels) 50s
RGB composite
Oxygen
Carbon
Nitrogen
Courtesy John Hunt, Gatan
9
Energy-Filtering TEM
  • Images of only a small range of energies
  • Energy window of 1-100eV
  • Just above or just below energy-loss edge
  • EFTEM compositional mapping
  • Elemental maps using multiple energy-filtered
    images
  • 2 images to determine background before edge
  • Scale background and subtract to obtain elemental
    signal
  • 1 image to collect elemental signal (edge above
    background)
  • Only one electron energy can be precisely in
    focus
  • All other energies will be suffer resolution loss
    (blurring)
  • The blurr is given by
  • d Cc b DE/E
  • Cc chromatic aberration constant
  • b the acceptance angle of the objective
    aperture
  • DE range of energies contributing to the image
  • Blurr will be especially large for thick, high-Z
    specimens.

10
EFTEM Elemental Mapping
  • Three-Window Method
  • Subtract edge background using two pre-edge
    images (dotted line)
  • Element concentration proportional to area of
    edge above background (outlined in red)
  • Absolute concentration can be determined if
    thickness and elemental cross-sections are known

Courtesy John Hunt, Gatan
11
EFTEM Elemental Mapping Example 1
Aluminum
Titanium
6 layer metallization test structure 3 images
each around O K edge _at_ 532 eV Ti L23 edge _at_
455 eV Al K edge _at_ 1560 eV
1 µm
Oxygen
Superimpose three color layers to form RGB
composite
O
Al
Ti
Courtesy John Hunt, Gatan
12
EFTEM Elemental Mapping Example 2
N
BF image
Color composite of all 5 elemental maps displayed
on the left,showing the device construction.
Unfiltered bright-field TEM image of
semiconductor device structure and elemental maps
from ionization-edge signals of N-K, Ti-L, O-K,
Al-K, and Si-K.
Courtesy John Hunt, Gatan
13
EFTEM detection limits
  • Typically 2-5 local atomic concentration of most
    elements
  • 1 is attainable for many elements in ideal
    samples
  • 10 for difficult specimens that are thick or of
    rapidly varying thickness
  • Sensitivity limited by
  • Diffraction contrast
  • Small number of background windows
  • Signal-to-noise
  • Thickness
  • Artifacts
  • If you can see the edge in the spectrum, you can
    probably map it
  • EFTEM spectrum image can map lower concentrations
    than the 3-window method
  • Better background fits because there are more
    fitting channels

Courtesy John Hunt, Gatan
14
STEM EFTEM EELS Spectrum Imaging
15
STEM spectrum image acquisition
  • The spectrum image data cube is filled one
    spectrum column at a time
  • In STEM it is possible to collect x-ray, EELS,
    BF, and ADF simultaneously
  • Use of the ADF or SE signal during acquisition
    permits spatial drift correction
  • STEM spectrum image
  • acquired by stepping a focused electron probe
    from one pixel to the next

EDX
Courtesy John Hunt, Gatan
16
EFTEM spectrum image acquisition
  • EFTEM spectrum image
  • Acquire an image containing a narrow range of
    energies
  • The spectrum image data cube is filled one energy
    plane at a time
  • Image plane retains full spatial resolution of
    TEM image

Courtesy John Hunt, Gatan
17
STEM EELS spectrum imaging
  • EELS STEM SI acq. at 200keV (cold FEG)
  • xy 5029 pixels
  • E 1024 channels (75eV, D0.5eV)
  • Acquisition time 5 minutes
  • Processing time 5 minutes

Courtesy John Hunt, Gatan
18
Quantitative EFTEM Spectrum Imaging
  • EFTEM Spectrum Image
  • 2.9 nm resolution
  • Si-L23 75-150eV3eV steps (1.5 min)
  • N-K, Ti-L, O-K 350-650eV
    5eV steps (8 min)
  • FEI CM120 BioFilter
  • 120keV
  • Corrections x-rays, MTF, spatial drift
  • Scaled by hydrogenic x-sections

Courtesy John Hunt, Gatan
19
STEM vs. EFTEM Spectrum Imaging
  • Quantitative elemental mapping
  • Both STEM SI and EFTEM SI can do this
  • EELS STEM Spectrum Imaging
  • Good quality spectra
  • All artifacts / instabilities correctable
  • Usually safer w/unknowns
  • EFTEM Spectrum Imaging
  • Fast mapping
  • Uncorrected artifacts / instabilities are very
    dangerous
  • Very useful for well characterized systems
  • Excellent spatial resolution

20
X-ray Spectrum Imaging
21
Mining the SI Data Cube
Multivariate Statistical Analysis of X-ray
Spectrum Images
Nb(wt)
Nb(wt)
1.5
1.5
0
0
  • Masashi Watanabe
  • Lehigh University

22
X-ray Spectrum Imaging
Specimen Ni-based superalloy
Collection of SI Huge data set e.g. 256x256
65,536 spectra each spectrum 1024 channels
cannot analyze manually Noisier spectrum
for XEDS than EELS Many possible variables
composition, thickness, multiple phases
100 nm
NiKa
AlKa
CrKa
What can we do?
TiKa
FeKa
Courtesy M. Watanabe
23
Multivariate Statistical Analysis
  • Multivariate statistical analysis (MSA) is a
    group of processing techniques to
  • identify specific features from large data sets
    (such as a series of XEDS and EELS spectra, i.e.
    spectrum images) and
  • reduce random noise components efficiently in a
    statistical manner.
  • Problems for which MSA may be useful
  • Investigation of data of great complexity
  • Handling large quantities of data
  • Simplifying data and reducing noise
  • Identifying specific features (components) can be
    interpreted
  • in useful ways

  • E.R. Malinowski, Factor Analysis in
    Chemistry, 3rd ed. (2002)

24
Nb map in Ni-base superalloy
MSA-processed
original
Nb(at)
Nb(at)
1
1
100 nm
0
0
  • Multivariate Statistical Analysis
  • identify specific features in the spectrum image
  • reduce random noise

Courtesy M. Watanabe
25
The Data Cloud
  • Find greatest variancein data
  • x1, x2, x3 are first three channels of spectrum
    or image
  • Manipulate matrices
  • Principal component analysis finds new axes for
    data cloud that correspond to the largest changes
    in the data
  • These few components can represent data

26
Principal Component Analysis (PCA)
PCA is one of the basic MSA approaches and can
extract the smallest number of specific features
to describe the original data sets.
The key idea of PCA is to approximate the
original huge data matrix D by a product of two
small matrices T and PT by eigenanalysis or
singular value decomposition (SVD)
D T PT
D original data matrix (nX x nY x nE) T score
matrix (related to magnitude) PT loading matrix
(related to spectra)
Courtesy M. Watanabe
27
Practical Operation of PCA
eigenanalysis or SVD
original data
loading
score
nE
nE
nE
nX
D
T
PT
line profile
PCA

nX

nY
nX x nY
nX x nY
eigenvalues
nE
D original data matrix (nX x nY x nE) T score
matrix (related to magnitude) PT loading matrix
(related to spectra)
D T PT
spectrum image
Courtesy M. Watanabe
28
Spectrum Image of Ni-Base Superalloy
matrix
NiKa
FeKa
CrKa
g
NiKa
NbLa
AlKa
TiKa
M23C6
CrKa
  • spectrum image
  • 256x256x1024
  • dwell time 50 ms
  • 20 eV/channel

Reconstructed spectra
Courtesy M. Watanabe
29
Results of PCA 1
Loading
Score
STEM-ADF
1 average
Ni Ka
Cr Ka
200 nm
2 M23C6
scree plot
Cr Ka
Ni Ka
3 g
Fe Ka
Ni Ka
Cr Ka
Noise
Al Ka
Ti Ka
Courtesy M. Watanabe
30
Results of PCA 2
Score
Loading
STEM-ADF
4 absorption
Cr Ka
Ni Ka
Ni La
200 nm
5 noise
scree plot
6 noise
Noise
Courtesy M. Watanabe
31
Comparison of Maps
Al
Nb
wt
wt
2
1.5
Original
0
0
wt
wt
2
1.5
Reconstructed
0
0
100 nm
Compositional fluctuations below 2 wt can be
revealed
Courtesy M. Watanabe
32
Application to Fine Precipitates
Irradiation-induced hardening in low-alloy
steel is caused by fine-scale precipitation Averag
e precipitate size 2-5 nm X-ray mapping in VG HB
603 300 keV STEM
BF-STEM image
ADF-STEM image
100 nm
Burke et al. J. Mater. Sci. (in press)
33
Application to Fine Precipitates in Steel
Burke et al. J. Mater. Sci. (in press)
Thickness
STEM ADF
Fe
Cr
50nm
5
1
20
85
95
10
(wt)
(wt)
(nm)
Ni
Mn
Cu
Mo
1
0
8
2
3
0
0.5
0
(wt)
(wt)
(wt)
(wt)
Too noisy
34
Application of MSA to Fine Precipitates
Burke et al. J. Mater. Sci. (in press)
Cr
Thickness
STEM ADF
Fe
50nm
5
85
95
1
10
20
(nm)
(wt)
(wt)
Ni
Mn
Cu
Mo
1
0
1.5
3
8
0
0.8
0
(wt)
(wt)
(wt)
(wt)
35
Some References to MSA Procedures
  • Multivariate statistical analysis in general
  • S.J. Gould The Mismeasure of Man, Norton, New
    York, NY, (1996).
  • E.R. Malinowski Factor Analysis in Chemistry,
    3ed ed., Wiley, New York,
  • NY, (2002).
  • P. Geladi H. Grahn Multivariate Image
    Analysis, Wiley, West Sussex,
  • UK,
    (1996).
  • For microscopy applications
  • P. Trebbia N. Bonnet Ultramicroscopy 34
    (1990) 165.
  • J.M. Titchmarsh S. Dumbill J. Microscopy 184
    (1996) 195.
  • J.M. Titchmarsh Ultramicroscopy 78 (1999) 241.
  • N. Bonnet, N. Brun C. Colliex Ultramicroscopy
    77 (1999) 97.
  • P.G. Kotula, M.R. Keenan J.R. Michael MM 9
    (2003) 1.
  • M.G. Burke, M. Watanabe, D.B. Williams J.M.
    Hyde J. Mater. Sci. (in press).
  • M. Bosman, M. Watanabe, D.T.L. Alexander, and
    V.J. Keast Ultramicroscopy


  • (in press)

36
Summary
  • Spectrum Imaging
  • the way serious microanalysis should be done
  • Mining the data cube
  • MSA is applicable for large data sets such as
    line
  • profiles and spectrum images
  • The large data sets can be described with a few
  • features by applying MSA
  • PCA is useful for noise reduction of data sets.
  • Be aware -- MSA can provide only hints of
    significant
  • features in the data sets (abstract components)
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