E-beam Characterization: a primer Part 1
Transcript of E-beam Characterization: a primer Part 1
E-beam Characterization:
a primer Part 1
Matthew J Kramer225 Wilhelm
October 30,2009
Why and Which Method•
E-beam characterization–
IT IS
the only reliable means for microstructural
and microchemical
analysis!•
E-beam Instruments–
Surface•
SEI –
From mm to nm, surface information only
•
BSE–
Surface Z distribution–
Topography
–
Transmission•
Diffraction contrast–
Microns to atoms•
Crystallography•
Both types can utilize the various spectroscopes
What do you need to know?•
Surface scanning–
Loose powders to polished surfaces
•
Large depth of field
–
Morphology will effect spectroscopy
•
Transmission Microscopy–
Region of interest needs to be electron transparent
•
~10 –
100 nm, depending on Z
•
How you thin can matter–
Significantly higher resolution
•
Very different imaging contrast used
The SEM•
E beam is accelerated by a large voltage
•
Lens forms a fine probe
•
Rastered
across the sample–
SEI
–
BSE
Imaging•
Secondary Electrons–
Very near surface
•
Backscattered Electrons–
Strongly Z dependent
–
Interactions at a depth 0
0.1
0.2
0.3
0.4
0.5
0.6
0 10 20 30 40 50 60 70 80 90
Z
e(BS
)/e(in
cide
nt)
Co-Sm-Fe alloy
CrystallographyBSE can be induced to channel along
crystallographic planesElectron Backscattered Diffraction (EBSD)
e interactions–
Auger electrons
•
Two views of the Auger process. (a) illustrates sequentially the steps involved in Auger deexcitation. An incident electron creates a core hole in the 1s level. An electron from the 2s level fills in the 1s hole and the transition energy is imparted to a 2p electron which is emitted. The final atomic state thus has two holes, one in the 2s orbital and the other in the 2p orbital. (b) illustrates the same process using spectroscopic notation, KL1
L2,3
.
Auger e’s
vs
X-rays•
Counter yield
•
Auger e’s
low energy–
Require a high vacuum
–
Very near surface
0.01 x 0.01 x 0.002 μ(10 x 10 x 2 nm )200 x 200 μ
Sample being analyzed
1 μ3
XPS AES
EDS
Depth: 0.002 -
0.01 μ (2-10 nm) 5-20 atom layers
NOTE: Scaling is only approximate
Detecting and Quantifying X-rays•
Wavelength Dispersive Spectroscopy–
Much higher energy resolution
0
500
1000
1500
2000
2500
3000
3500
4000
4500
5000
2.15 2.20 2.25 2.30 2.35 2.40 2.45 2.50E [keV]
coun
ts (a
rbitr
ary
units
)
S (WDS)Mo (WDS)S (EDS)
S eparatio no f M o Lαfrom S Kα14.3 eV
E D S en erg y reso lu tion
120eV FW H M
WDS energyresolution
3.45eV FWHM
0
25
50
75
100
0.6 0.7 0.8 0.9 1.0
distance (µm)
at %
AlGe
Quantification and Spatial Resolution
0
25
50
75
100
0 1 2
distance (µm)
at %
AlGe
1 µm
•
Average Z and E dependent
•
Requires stable e-beam source
•
Requires standardization
•
Requires known geometry–
i.e., flat, parallel surface
JEOL 5910lv •
Resolution (SEI) –
3.0 nm @30kv, 8 mmwd
•
Magnification –
18-300,000 x•
Probe Current–
1pa
1 microamp•
Image modes:–
SEI–
3 Backscatter•
Topo•
Compo•
Shadow•
EDS–
Line scans–
mapping
JEOL 5910lv•
Poor Vacuum mode:–
Resolution 4.5 nm @30kv, 5 mmwd–
Backscattered mode only in the poor vac
mode–
Adjustable chamber pressure 10-270 Pa
•
Tungsten filament with automatic adjustments
Beam Blanked in “Freeze”
mode
•
Alignments and conditions automatically and individually saved for each user
•
Specimen Chamber and Stage:–
5 axes (X 125mm range, Y 100mm range, Z 43mm range, T 10 to 90 range, R 360 endless)–
Maximum specimen size 7”
with full coverage–
Specimen position graphical indicator as well as chamber camera–
Absorbed current ( Specimen current ) measured
•
Image memory selectable to 1,280 x 960 x 8 bits
Can frame average
up to 255 frames
Image storage formats BMP, TIFF or JPEG.
–
We recommend BMP with merged text.
JEOL JXA-8200 Superprobe combined WDS/EDS
•
5 wavelength-dispersive spectrometers, 10 crystals
–
B through U–
four 140 mm Rowland circle
–
one 100mm Rowland circle
•
EDS, 10 mm2
Si(Li) crystal, Be window
–
Na through U•
Software –
quantitative analysis –
compositional mapping –
phase analysis–
integrated WDS/EDS operation.
Crystal K lines L lines
LIF (140mm) Ca – Rb Sn – U
LIF (100mm) Ca – Ge Sb – Hg
PET (140mm) Si – Fe Rb – Tb
PET (100mm) Si – Ti Rb – Ba
TAP O – P Cr – Nb
LDE1 (2d=60Å) C, N, O, F •
LDE2 (2d=90Å) B, C, N, O •
Overall Capabilities•
Electron Optical and Vacuum Systems–
W or LaB6 electron source–
Acceleration voltage 0.2-30kV–
Useable beam current 10-12 to 10-5A–
Pneumatically driven Faraday cup for beam current measurement (serves as beam blanking)–
Turbomolecular
vacuum pump–
All functions controlled through central computer system•
Imaging Capabilities–
Secondary electron detector–
Backscattered electron detector with composition/topography mode–
10 user selectable scan speeds–
Magnification 40x to 300,000x–
Optimal imaging resolution 6nm–
Dedicated 18 inch flat panel display for electronic images–
Optical microscope for reflected light observation of sample–
Optical system coaxial with electron beam–
High resolution color video mini camera–
Automatic optical focus device
Sample Preparation•
Maximum sample size–
150 x 150 x 50mm–
4 x 1in. diameter samples
•
Stage travel –
x = 100mm, y = 90mm, z = 3mm
•
Stage tracking–
< ±1μm
•
Requires flat, well polished surface
•
Standardization–
Elemental or line compounds
JAMP7830F Auger Microprobe
•
Schottky
field emission gun•
0.5 to 25kV beam voltage•
10-11
to 1x10-7
A current•
Minimum probe size: –
4 nm in SEM mode, –
10 nm in Auger mode•
Chamber pressure–
5 x 10-8
Pa (3 x 10-10
torr)•
Stage movement: –
X,Y + -
10mm, Z + -
6mm•
Normal sample size: –
12mm dia. 5mm thick
JEOL 7830F AES Advantages & Capabilities ( HSA vs CMA, and FE vs LaB6 )
Key Components
that produce
High Energy
Resolution and Reliable
KE Values
JEOL 7830F Schematic View
High Energy Resolution AES Chemical State Map:
SEM
Cu2 OCuo
Red = Cuo
Green = Cu2 O
•
Cuo
vs
Cu2
O (Δ E = 0.9 eV)
Chemical Shifts
O
CrOx
Cro
CrOx
Cro
This sample was ion etched to remove all
contamination and left in UHV at 3 x 10-10 torr
14 hr.
This reveals the reactive nature of “clean”
surfaces.
O hr -
start
14 hr -
end Gas Capture Study
•
Reactive Nature of the Clean Surface of a Co-Ni-Cr Alloy
Limitations of Auger Electron Spectroscopy•
Cannot detect hydrogen or helium
•
Destructive depth profiles.•
Samples must be small and compatible with high vacuum.
•
Elemental quantization depends on instrumental, chemical, and sample related factors.
•
Chemical information is depended on quantity and element
•
Most sample surfaces are contaminated—must be cleaned by ion etching
Sample Preparation•
Best if sample is parallel polished
•
Best sample size:–
< 10 mm dia.
–
< 3 mm thick•
Please no potting of sample in plastic matrix
•
For very small samples consult with us first•
Samples that are used in some type of process, need to be in proper form before processing
•
Remember ----
do not touch the samples with your hands!
Conclusions•
1st
determine what you need to know–
i.e., grain size or just average chemistry–
How precise do your measurements need to be?•
Will dictate sample preparation, obtaining standards etc.•
WDS vs
EDS or is BSE good enough–
What elements are possibly present, including impurities?•
Are there overlaps? WDS vs
EDS–
Chemistry of the surface or of the bulk?•
XPS and SAM vs
SEM•
Decide which instrument(s) will be needed–
Discus techniques and sample preparation first with staff•
Not with your classmates (unless they are an expert)!•
Keep an open mind–
It is not unusual that your preconceived notions are wrong–
But artifacts are possible•
How does grinding and polishing affect the composition and possibly microsctucture•
Is your sample sensitive to air, moisture etc.•
How do these results mesh with other bulk measurements?–
Microscopy is a powerful tool, but one of many tools, it should be complimented with other techniques when appropriate.
•
XRD, SQUID etc.