saed patterns of single crystal, polycrystalline and amorphous samples abc r1r1 r2r2 200 020 110

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SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples a b c r 1 r 2 200 020 110

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Page 1: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples

a b c

r1 r2200

020

110

Page 2: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Electron Diffraction

Specimen foil

T D

e-

L 2

r

dhkl

[hkl] SAED pattern

L -camera lengthr -distance between T and D spots1/d -reciprocal of interplanar distance(Å-1)SAED –selected area electron diffraction

Geometry fore-diffraction

Bragg’s Law: = 2dsin

=0.037Å (at 100kV)=0.26o if d=4Å

= 2dr/L=sin2as 0r/L = 2

r/L = /d or

r = Lx1

d

hkl

Reciprocal lattice

Page 3: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Ewald’s Sphere

Ewaldcircle

0

incident beam

diffracted beam

2

C

ki Gg

130

H

Ewald’s sphere is built for interpreting diffraction

CG-C0=0G or kd-ki=g Laue equation

lkl=1/

kd

Wherever a reciprocal lattice point touches the circle, e.g., at G, Bragg's Law is obeyed and a diffracted beam will occur. At H, no diffraction.

Page 4: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Convergent Beam Electron Diffraction (CBED)

CBED uses a conver-gent beam of elec-trons to limit area of specimen which con-tributes to diffractionpattern.Each spot in SAED thenbecomes a disc withinwhich variations inintensity can be seen.CBED patterns containa wealth of informationabout symmetry andthickness of specimen.Big advantage of CBEDis that the informationis generated from smallregions beyond reachof other techniques.

Page 5: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

SAED vs CBED

spots disks

lens

sample

Parallel beam Convergent beam

T D T D

Convergence angle

objective

SAED CBED

Spatial resolution >0.5m

Spatial resolutionbeam size

Page 6: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

CBED-example 1

Page 7: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

CBED-example 2

HOLZ

HOLZ - High Order Laue Zone

Page 8: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Applications of CBED

•Phase identification•Symmetry determination-point and

space group•Phase fingerprinting•Thickness measurement•Strain and lattice parameter measurement •Structure factor determination

Page 9: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Symmetry Deviations

Page 10: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Phase Identification in BaAl2Si2O8

200oC 400oC 800oC

<0001>

Hexagonal Orthorhombic Hexagonal

6mm 2mm 6mm

Page 11: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Phase Fingerprinting By CBED

[001] CBEDpatterns of anantiferroelectricPbZrO3 singlecrystal specimenat (a) 20oC, (b)280oC, (c)220oC.(d) [001] CBEDpattern of a rhombohedral ferroelectric Pb(ZrTi)O3 Specimen at 20oC.

Orthorhombic AFE Cubic PE

Rhombohedral FE Rhombohedral FE

Page 12: SAED Patterns of Single Crystal, Polycrystalline and Amorphous Samples abc r1r1 r2r2 200 020 110

Symmetry and Lattice Parameter Determination

BFEDS

[143]

[100]

[111]

CBED

CBED-HOLZ

Experimental simulated

Latticeparameters

SAED

010

001

0.2m

NbA

B

A

A

A

A

B

B

B

B