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8/14/2019 GholiniaEBSDOverview
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www.hkltechnology.com
Electron Back-Scatter Diffraction in
the Scanning Electron Microscope:
An Overview
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What is EBSD?
Historical Perspective
Crystallography & pattern formation
Data Collection
Recent Developments Conclusions
al! "utline
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What is EBSD?
EBSD # electron $ac!scatter %iffraction
SE $ase% techni'ue to measure crystal
orientations
(pplica$le to any crystalline material )in theory*
Provi%es the a$solute crystal orientation +ith su$#
micron resolution
( useful tool for %iscriminating $et+een phases
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EBSD or EBSP?
EBSD# electron $ac!scatter %iffraction
EBSP, electron $ac!scatter %iffraction pattern
BKD, Bac!scattere% -i!uchi Diffraction
And some commercial names....
(C)OM, )Crystal* "rientation apping
ACOM, (utomate% Crystal "rientation
apping OIM. # "rientation /maging icroscopy
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What is EBSD?
Historical Perspective
Crystallography & pattern formation
Data Collection
Recent Developments Conclusions
al! "utline
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EBSD History ,Early Wor!
EBSP li!e patterns +erefirst o$serve% $y-i!uchi )0123* in theransmission Electronicroscope )E*4
5on Boersch )0167*e8ten%e% -i!uchi9s+or!
Mica
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EBSD History ,
(lam et al4 (lam: Blac!man an%
Pashley )01;: -/:
aCl: P$S2
crystals4
Lead Sulphide
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EBSD History , the $irth of
mo%ern EBSD 5ena$les an% Harlan%
)0172* o$serve% EBSPs inthe Scanning Electronicroscope )SE* $y usinga 6@mm %iameter fluorescentimaging screen an% a close%circuit television camera4
Dingley )later 013@s*%evelope% the com$ination
of phosphor an% televisioncamera: an% com$ine% them+ith a graphical overlay4
EBSP from Dingley'sgroup note
calibration marks
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EBSD History , continue%
e8periments in the 013@s Commercial soft+are
)0131* +as %evelope%
to analyse ElectronChanneling Patterns)ECP* an% EBSPs4
E film for high'uality EBSPs & phase
i%entification )013@s*
EBSP from a superalloy collected with EM film
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EBSD History , commercial
systems in the 011@s (utomatic metho%s for
in%e8ing EBSPs)011@s* an% control of
SEs gave rise tomapping an% phase%iscrimination4
Digital cameras: EDA%ata an% phase%ata$ases provi%einformation for phasei%entification )0111 # * Phase map from
duple steel
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EBSD History , the present %ay
High spee% mapping$ecomes a reality
DualCross $eam
system )Electron /on$eam* for 6Dmicroscopy
Com$ine% chemical an%crystallographicmapping
!rientation map of "i#superalloy$ collected at
%& points ( sec
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EBSD set up
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Resulting %iffraction pattern
)EBSP*
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EBSD
Performance
Spatial resolution %o+n to 0@s of nm
Max sample size SE %epen%ent )typically
up to 0@@ 8 ;@mm*Angular resolution @42;#0 at present
Probe current F@42; n(
Accelerating voltage F; !5
Specimen tilt G@#7;
Working distance 0@#
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What is EBSD?
Crystallography & pattern formation
Data Collection
Recent Developments
Conclusions
al! "utline
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EBSP symmetry comes from lattice symmetry
, Crystal system: =aue group: space group
o $uil% a crystal
, Start +ith unit cell
, (%% a $asis
, Repeat a% infinitum444
uv+I is a crystal %irection:
Juv+F is a family of %irections
)h!l* is a crystal plane:
Kh!lLis a family of planes4
EBSP crystallography
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EBSP formation
Spherical
-i!uchi map
Phosphor
Electron $eam stri!esspecimen
Scattering pro%uceselectrons travelling in all%irections
Electrons that satisfy theBragg con%ition
)nM2%4sin* for a plane)h!l* are channele% -i!uchi $an%s
Electrons stri!e thephosphor an% pro%uce light
Which is %etecte% $y a CCDcamera an% %igitise%
he resulting EBSP isautomatically analyse% an%in%e8e%444
/ron unit cell
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(lthough EBSPs are create% $y
$ac!scattere% electrons: the signal
%oes not come from the +hole BSE
interaction volume
/nstea%: the %iffraction signal
effectively originates from a Npoint
sourceN in the top fe+ nm
his means that the EBSD
techni'ue can o$tain very high
resolutions )J2@nm*
EBSD Resolution
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Copper interconnect test
sample (nalyse% on the =E" Supra
;;5P
Resolution E8ample 0
Twin domain !"#$" nm
wide a%e clea%ly
%eol&ed 'ing a nm
te i*e
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Pt thin film
(nalyse% on the OE"=G;@@>
Resolution E8ample 2
+%ain with a mean
diamete% o, -nm a%e
clea%ly %eol&ed 'ing a
nm te i*e
=0.08 m; BC; Step=0.005 m; Grid55x49
=0.08 m; GB+tri-x; Step=0.005 m; Grid55x49
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{100}
[100] [010]
[011]
[001]
{110}(011)
!"
[100]
[001]
[111]
[101]
[201]
[311]
[210]
[011]
[110][010]
Bo%y centre% cu$ic /ron
/ron EBSPJ000F is central
ote J000F has 6
fol% symmetry: $ut is
close to G fol%4
{#00}
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$cc
fcc
82
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Differences in interplanarangles allo+ similar
loo!ing EBSPs from$cc
an% fcc/ron to $e
%istinguishe%4
$cc /ron fcc /ron
$cc /ron fcc /ron
Phase %iscrimination
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What is EBSD?
Crystallography & in%e8ing
Data Collection
Recent Developments
Conclusions
al! "utline
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A ingle a'tomated EBSD %'n %o&ide a
completecha%acte%iation o, the mic%ot%'ct'%e2
Phase %istri$ution
e8ture strength
Qrain sie
Boun%ary properties
isorientation %ata
Slip system activity
/ntra#granular %eformation Plus much: much more
all provided !ile you get on it! somet!ing else..."
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3o%ked e0amle o, a'tomated
EBSD(nalysis of polycrystalline samples of halite
)aCl , cu$ic*
Some samples have $een e8perimentally%eforme%
5ariations in grain sie an% in e8tent of
su$grain %evelopment necessitate analysis at
%ifferent scales
#ata source: $trec!t $niversity% using a P!ilips &'() *+,
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Stage can
o%ientation ma o,
olyc%ytallinehalite
0@@0@@ gri%: step 0@@ m4
< mm
(nalysis time
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;@@ m
6@@6@@ gri%: ; m step
Beam can o%ientation
ma o, olyc%ytallinehalite
(nalysis time 6G minutes
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Stage scan: 6;@6@@ gri%: 2;m spacing
64; mm
Compression
/a%ge a%ea can
o, olyc%ytalline
halite
EBSD on di,,e%ent cale I
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2@@ m2@@ m
A
B
Beam scan: 2;@2;@ gri%: 24; m spacing
-ieing intragrain microstructure and local lattice orientation variations...
Reflecte% light image
EBSD on di,,e%ent cale II
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@
0
2
6
/B an% electron $eam*
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EBSD %etectors
=o+ light EBSP camera, Silicon intensifie% target )S/*
3 $it: very noisy
, CCD , 5 type vi%eo signal3 $it less noisy
, Slo+ scan CCD02 $it: lo+ noise: high spee%: $inning
Binning /ncreases signal: re%uces noise
Higher spee% $ut at lo+er resolution
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EBSPs # >el%spar
"l% Camera e+ Camera
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Halite # aCl
020:2@< points
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6D#EBSD
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What is EBSD?
Crystallography & in%e8ing
Data Collection
Recent Developments
Conclusions
al! "utline
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Conclusions
EBSD is an SE#$ase% techni'ue that has $een
!no+n for ;@ years: $ut only +i%ely applie% in the
last 0@ years
EBSD is no+ a fast: automate% techni'ue:applica$le to most crystalline materials
EBSD provi%es phase i%entification: te8ture an%
$oun%ary characteristics44444