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