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Elastic Scattering and Kinematic Theory of Electron Diffraction
Dr. Hongzhou Zhang [email protected]
SNIAM 1.06 896 4655
Lecture 2
• Elements of the TEM
• Simple pictures of how to acquire images and diffraction patterns - Modes
• Alignment of the TEM
Reminder: Homework 1:Lecture 4 (due at lecture 5): Find a paper… please start looking for papers…
Content
• Signals in the TEM
• Elastic Scattering
– Quantitative description of the scattering process
– Atoms, Unit cells, Crystals
• Kinematic Theory of Electron Diffraction
– Geometrics of diffraction patterns
– Reciprocal lattice
Signals in a TEM
Specimen
Backscattered e
Secondary e Auger e
X-rays Cathodoluminescence
Incident e beam
Un-scattered e Inelastically Scattered e
Elastically Scattered e
Induced current
e, h pairs
Signals: Consequences of scattering processes
Scattering: Duality
• The natures of the scattering: interaction, energy exchange, …
• Scattering probability • Angular distribution of the
scattered waves/particles – Intensity – Amplitudes/phase
• Mean Free Path
Particle perspectives
Wave perspectives “Signals”
Atoms – Unit cells – Crystal
Coherent scattering:
Incoherent scattering:
j
j
r
rcoh
2
* j
j
r
rcohcohcohI
j
j
r
rincI
2
elastic inelastic
Coherent Diffraction, image contrast Neutron scattering – excitations (phonons, magnons)
Incoherent No sharp crystal-structure-related diffraction Broad angular dependence Compton scattering
Spectroscopies Absorption Analytical: EELS/ELNES/EXELFS
The incident – a precise phase relationship – The scattered
Scatterings: Different types
- Interactions: Single/plural/Multiple Single Scattering (Kinematic): not even for thin sample of ~nm Multiple-scattering: e-probe broadening
• Elastic: the solid remains in its original state - Total kinetic energy and momentum conserved - Coulomb atomic potential/screened (small angle scattering)
• Inelastic: excitation of energy states E = Ef-Ei
- Electron-electron interaction - Less localized processes
This is not all about using a coherent source
Differential cross section: Particle Perspectives
a: Impact parameter
Hyperbolic trajectories
2: scattering angle
a decreases
2 increases
Differential cross section:
I
I
IFlux density of the incident beam:
The electron flux scattered per solid angle:
I
d
d
I: # of electrons per unit time
• Anisotropic scattering:
beamincident theofdensity flux The
d angle solidper scatteredflux electron The section -cross lDifferenta
Angular distribution of scattered particles
• Total cross section:
s
dd
d
S
r
For a given , I
increases
d
dDecreases, a function of
Angular distribution
Scattering Potential
Scattering Length/amplitude: Wave Perspectives
rkiri
exp0
• Incident plane wave
• Scattered spherical wave
rrikrr
fikrr
frsc
expexp 00
f() ~ dimension of length
rrr si
• The total field
- Far from the scattering centre, r >> r’
Spherical wave ~ plane wave
rrkir
r
exp1
4
1
Cross-sections and scattering length
**
2m
hiej
2
00**
02
Ψm
ke
m
iej iiii
2
03
0**
2Ψf
r
r
m
ke
m
iej sssssc
rkiri
exp0Incident plane wave:
Scattered spherical wave: ikrr
frrikrr
frsc expexp 00
0
0
Charges passing through d :
Wave Perspectives :
2
f
d
d
djdrjsc 0
2 0
2
j
jr
d
d sc
Particle Perspectives: dS
dIj
d
dIj 0
djdI 0
The current, dI, scattered passing through solid angle d
dr
dI
dS
dIjsc 2
drjdI sc
2
f() ~ dimension of length
Current intensity: Charge conservation
ip̂
Scattering amplitude/length/factor: Wave perspectives
rErrVm
)(
2
22• The Schrodinger equation: rrV
mr
mE )(
2222
2
rrUrk )(2
0
2
A point source at r’ : rrikrr
rrG
exp1
4
1,
Satisfies the equation: '',2
0
2 rrrGk
• The amplitude of the total scattered wave • Sum of the amplitude of spherical waves from scattering centres • Scattering centres: Electrons of the atoms, atoms of the crystal
The weight of the spherical wave centred at r’: rrU )(
The total scattered amplitude: rdrrGrrUrs
3,)(
rdrrGrrUrs
3,)(
The asymptotic solution far from the nucleus (the detectors)
Spherical wave ~ plane wave rrkir
rrG
exp1
4
1,
rdrkirrVr
rkimrs
3
02exp)(
exp
2
The first Born approximation: single scattering rkir
00 exp
rdrkkirVr
rkimrs
3
002exp)(
exp
2
Coherent scattering
V(r): atomic, crystal,… )(
2)(
2rV
mrU
For each scattering, the wave before the scattering is the incident plane wave
The scattering factor
r
ikrfs
exp0
rdrkkirVr
ikrmrs
3
020 exp)(exp
2
• Scattered wave:
rdrqirVm
rdrkkirVm
f 3
2
3
02exp)(
2exp)(
2
0
0
22 2
2
2 EE
EE
E
m
• To work out f(), using the interaction potential:
2
4
0
3
0
3
0
2
2
expexp
42
q
j
j
fZ
jjj rdrr
rriqrdrqirZ
emf
x
sin20 kkkq
xfZh
mef
2
2
2
0 sin24
1
r
Zedr
rr
redrrrrVrV j
j
j
ij
22
0
1
)(
4
1...)...;(*)(
0kkq
Cross sections: Large angle ( fx = 0) Rutherford cross section:
2
2
2
0
2
22
sin
1
8
mv
Zef
d
d R
Small angle cross section: 4
2 1~
fd
d el
2 k0
k
Definition of the scattering factor:
For an atom:
Model potentials:
R
r
r
ZerV exp
4)(
0
2
3
1
ZaR H nm0529.0Ha
Wentzel model (screened Coulomb Potential)
Discussion on f()
Strongest in the forward direction, i.e. small scattering angle: coherent, constructive in the forward direction
Stronger for lower beam energy, i.e. longer
wavelength
f() is normally a complex number: additional phase
due to scattering
Length unit
Larger |f| for heavier atoms
xfZh
mef
2
2
2
0 sin24
1
• Born approximation: single scattering • Ignored: exchange effects, virtual inelastic scattering effects, spin, Bremsstrahlung energy losses, electron-induced damage, absorption
• Only can be measured for gas target: multiple scattering • WKB + muffin-tin model
• Atomic shell structure ignored Reimer, TEM, Springer
f(0): sensitive to the mean
inner potential
Total elastic cross section and mean-free-path length
dd
dd
d
del sin2
0
4
0
• The total elastic cross section per atom
2Rr
Billiard balls
• Total cross section (per atom) inelelt
• A layer of solid
• Scattering occurs when the electron strikes a portion of ds: dzdsNt
- The scattered fraction dj of j
• The current intensity of electrons remain unscatterred at z (direct beam) :
t
t
zjzNjj expexp 00
- The total mean-free-path length Nt
t
1
- Thickness, dz; Area, ds; volume: dzds
- # of Atoms: dsdzNA
dsdzN A
A
NN A
-123 mol1002.6 AN
A: the atomic weight
- Mass: dzds
dzNds
dzdsN
j
djt
t
Radiation Elastic mean free path (Å) Absorption length (Å) Probe size (Å)
Neutrons 108 109 107
X-rays 104 106 103
Electrons 102 103 1
2
f
d
d
Observable… … The strength of electron diffraction is 106 stronger than XRD
Carbon, organic materials, you
need 80kV beam
Energy Transfer in an Electron-Nucleus Collision
2
2
0' sin22
Mc
EEEEn
• The conservation of momentum
- Momentum of the nucleus: non-relativistic
- Momentum of the electrons: relativistic
nppp
nn EMp 2
2
021
EEEc
p 2
021
EEEc
p
• The conservation of energy nEEE
• The energy transferred
- Negligible for small
- For higher E and large
• Displacement energy: Ed 10-30 eV
Atoms being displaced from their lattice points: damage
• Knock-on processes: small cross section
• Threshold Ec: En=Ed, = 90o
dd
d elD
2/
min
sin
dn E
Mc
EEEE
min
2
2
0' sin22
d
ccn E
Mc
EEEE
2
022
ZoBelli, A. Gloter, C. P. Ewels, G. Seifert, C. Colliex, Electron knock-on cross section of carbon and boron nitride nanotubes, Physcial Review B 75, (2007). R. F. Egerton, R. McLeod, F. Wang, M. Malac, Basic questions related to electron-induced sputtering in the TEM. Ultramicroscopy 110, 991 (Jul, 2010). O. L. Krivanek et al., Gentle STEM: ADF imaging and EELS at low primary energies. Ultramicroscopy 110, 935 (Jul, 2010).
OK for elements on this side…
Diffraction in the TEM
• Selected Area Electron Diffraction (SAED) – >~100 nm
• Convergent-beam diffraction (CBED) – Each point: particular k
– Intensity across the disk ~ f(k)
– 1~10 nm
– Uniform: orientation and thickness
• Identity of Phase/orientation relationship
• Habit planes of precipitates, slip planes
• Exact crystallographic description of crystal defects
• Order/disorder, spinodal decomposition, magetic domains and similar phenomena
The one closest to that passes
the origin
Crystallography • You may want to review crystal structures …
• Chapter 1, Marc De Graef, Introduction to Conventional TEM, Cambridge • Chapter 1&2, Charles Kittel, Introduction to Solid State Physics, Wiley • Chapter 4-7, Ashcroft/Mermin, Solid State Physics, Brooks/Cole • Chapter 1-3, A, Kelly, et.al, Crystallography and Crystal Defects, Wiley • Gerald Burns/Am. Glazer, Space Group for Solid State Scientists, Academic
- Primitive cells
The origins of the unit cells: cobnamrg
The positions of atoms: czbyaxrk
0,0,01 r
2
1,
2
1,
2
12r
- Lattice Planes (miller indices): (hkl) The reciprocal intercepts in units of a, b, c
The intercepts in units of a, b, c
- Directions: [uvw]
Equivalent Directions: <uvw>
Equivalent planes: {uvw}
Braces/curly brackets
Angle brackets
Square brackets
Round brackets
The Assumptions of Kinematical Theory
• Monochromatic wave
• Plane waves (T, D)
• Free of distortion
• Negligible diffraction (all atoms receive an incident wave of the same amplitude)
• No interaction between T and Ds: Refractive index = 1
• No absorption
• No re-scattering of scattered waves
A geometrical Approach
• Diffraction of monochromatic light by a grating – Large distance R – In phase: path difference = n – → intensity : low
efficiency for large angle scattering
• Scattered wavelets – in phase in particular crystallographic directions – Scattering by an individual
atom f() – Scattering by a crystal
• Angular distribution – The Bragg law – The Laue Conditions – Structure &lattice
factors/amplitudes
The Bragg Law
d
Scattering angle: 2
T D
Bragg Law: simple method of visualising diffraction
• Crystal planes - Wavefront
• Path difference for strong diffraction
ndhkl sin2
The smallest angle: n =1 2
d
(1) Path difference: 2
sin
d
(1)?
(2)?
(2) Path difference: 2
332sinsin
ddd
(3)?
(3) Path difference: 243sinsin ddd
(4) n = 2
Diffraction along (1):
d 2
dd sin
Tilt the beam, and the diffraction tilts accordingly
Ap
pro
x.
Quantitative approach - Laue Conditions
nPr
• Scattering by individual atoms
• Incident/scattered waves: po, p (unit vectors)
• Path difference for constructive interference
Atoms: cwbvaur
0ppP
• Laue conditions for diffraction:
haP
2
2
kbP
2
2
lcP
2
2
The solution of the Laue conditions, k, satisfies the diffraction condition and defines diffracted beam k
po p
O B
A
A’ • Phase difference for constructive interference
nrP
2
2
hak 2
kbk 2
lck 2
0prOA
prAO
0pprAOOA
Path difference
00
2kp
kp
2
0kkk
ko k
k
b a
Laue Conditions: The solution • The solution
where ......;0;2;2;2 **** baccbbaa
Each point in reciprocal space: a set of particular planes in real space
Two vectors AB and BC in Plane (hkl)
0*****
bk
k
bah
h
aclbkah
k
b
h
aghkl
AB
0*****
bk
k
bcl
l
cclbkah
k
b
l
cghkl
BC
g
AB
)( plane hklghkl
g
BC
)( plane hklghkl
*** clbkahgk hkl
- Orthogonal axes (cubic, tetragonal, orthorhombic): Reciprocal Lattice coincide with Crystal lattice
cba
,*
k
b
OB
h
a
OA
l
c
OC
O
A
B
C
OAOB
OBOC
g d
aa 2*
- Properties
hkl
hkld
g2
gg
clbkah
h
a
g
gdhkl
2***
OA
c
a*
b*
c*
a
c
b
cba
cba
2*
hklgk
Diffraction
Laue Conditions and Diffraction
0k
k
gkkk
0
g O
L
G
• Construct the direction of diffraction beams
In the reciprocal space
- A line from L to O (the origin)
- in the direction of the incident beam
- Magnitude k0=2/
- A line from L to G (ghkl)
- Magnitude k=k0=2/
LG: The diffraction k due to the planes corresponding to ghkl
2
• The Bragg Law
hkl
hkld
gk
2
sin2 0
hkl
hkld
g
2sin
22
sin2 hkld
G2
hkl
hkld
ngnk
2
sin2 0 ndhkl sin2
nrg 2
Scattered by a Unit Cell – the Structure Factor
xfZh
mef
2
2
2
0 sin24
1
Atoms – Unit cells – Crystal
n
nnnn
n
nn lzkyhxififF 2expexp
• Unit cells
r
ikrfs
exp0
- Position of atom in the atomic plane czbyaxr nnnn
- Additional phase nnnnhklnn lzkyhxrgrP
2
2
• Atoms:
- Scattered amplitude factor by the cell:
Coherent Scattering, sum of the amplitude
0,0,01 r
2
1,
2
1,
2
12r
lkhiff
lzkyhxififF
AlNi
n
nnnn
n
nn
exp
expexp
- Intensity: 2FI
Nlkhff
Nlkhff
lkhfflkhff
FI
AlNi
AlNi
AlNiAlNi
2when
12when
2sincos
2
2
22
2
The same atoms
Nlkh
NlkhfFI
2when 0
12when 4 22
Systematic Absence
Systematic absence
d
T
D
A’ C’
For AA’-CC’ : sin2 )(hkld
Due to the addition scattering (200) A
C B
B’
For AA’-BB’ : 2sin
22
d
For BB’-CC’ : 2
sin2
2
d
No diffraction: 2
A’’ B’’ C’’
For AA’’-CC’’ :
243sinsin ddd
For AA’’-BB’’ :
For BB’’-CC’’ :
42
d
42
d
Diffraction beam: 4
1 2
3
(100) Systematic absence h+k+l =1 is an odd number
(200) Diffraction Occurs h+k+l =2 is an even number
Scattered by a Finite Crystal – Crystal Factor
Very thin samples: 100 nm ~ 500 unit cells
Atoms – Unit cells – Crystal
cnbnanr zyx
The origins of the unit cells:
- Additional phase
zgygxgnnn nznynxrgrP
2
2
zyx
zyx
NNN
nnn
zgygxg
n
n nznynxiFiFG
,,
,,
2expexp
- Scattered amplitude factor by the crystal:
X
XX
nN
n
nx
1
11
0
z
zz
g
yg
g
xg
iz
Niz
iy
Niy
ix
NixFG
2exp1
2exp1
2exp1
2exp1
2exp1
2exp1
- Intensity: 2GI
g
zg
g
yg
g
xg
z
Nz
y
Ny
x
NxFI
2
2
2
2
2
22
sin
sin
sin
sin
sin
sin
- Maximum: hxg kyg lzg hklgg
- Falls to zero: x
gN
hx1
;0sinsin ihihNNix xxg
Laue condition is relaxed!
Reciprocal Space
0k
k
g=ghkl+s
O
L
G
2
s
ghkl
g
zg
g
yg
g
xg
y
Ny
y
Ny
x
NxFI
2
2
2
2
2
22
sin
sin
sin
sin
sin
sin
sgg hkl
z
zz
y
yy
x
xx
s
Ns
s
Ns
s
NsFI
2
2
2
2
2
22
sin
sin
sin
sin
sin
sin
Perfect crystal: s varies slowly across the crystal
O
The Reciprocal lattice and Ewald Sphere
• Ewald sphere Construction
• Diffraction in 3D Specimen, Real space
Reciprocal space
- Choose a reciprocal lattice, O, as the origin of the lattice -A line from L to O (the origin)
- in the direction of the incident beam - Magnitude k0=2/
- A sphere centred at L, radius |k0| - The wavevectors k of all possible elastic diffracted waves emanating from L and terminated at the sphere
L
• The Ewald Sphere: – Radius of Ewald: 2/ ~ 17 nm-1 (100kV)
– Reciprocal lattice spacing: 0.3nm-1
– Flat surface: several streaks cut simultaneously
These g more or less perpendicular to the incident beam
Reciprocal Lattice: Laue Zones
nrg 2
*** clbkahg
cwbvaur
2* aa
nlwkvhu
0 lwkvhu rg
[uvw]
1g
2g
3g
• Zero-order Laue Zone:
The atomic planes (real space) have the zone axis as a common line of intersection
0rg
A plane in reciprocal space that is perpendicular to the beam
• high-order Laue Zone (HOLZ): 2rg
2
Beam direction r – real space
Selected Area Diffraction Optical Axis
k0 k
0k
k
Reciprocal Space
BFP of the OL
Image Plane of the DP R
hkl
hkld
g2
L
k
R
ghkl
LRdhkl
1212
LRdhkl
L : camera constant; L: camera length
...
8
31
2
L
R
R
Ldhkl
Projection lens imperfection makes is
unnecessary
Summary
• Atoms-Unit Cells-Crystal: Scattering factors
• Diffraction pattern: the spot array on the surface of the Ewald sphere
Reciprocal – Real Spaces
Real Space Reciprocal Space
SC SC
Tetragonal Tetragonal
Hexagonal Hexagonal
FCC BCC
BCC FCC
Elastic Scattering Amplitude f() - WKB method
rkirirar ss
00 expexp
rdrV
EE
EE
Erdrnrs
0
0
2
21
2
Near Field: Modification of the incoming plane wave
1expexpexpexpexp 000000 rirkirkirkiri ss
The scattering amplitude: rdrkkiriikf s
3
0exp1exp
Wave-front behind the atom:
No absorption: 1ras
Phase shift due to the atom using the electron-refractive index:
Rewrite the exit wave:
Incident: i
rkiri
00 expIncident wave:
Scattered: sc
Far field, Fraunhofer diffraction, k: ikr
rfrsc exp0
Weak phase specimens (s <<1): rdrqirkf s
3exp
Using refractive index:
rdrqirV
EE
EE
Ef 3
0
0
2exp
2
2
0kkq
Coherent Scattering
Cross-section by a single electron: 2
j
j
r
rf
d
d
Cross-section by an atom (Z electrons):
d
dZfZf
d
d jr
j
j
j r
Z
r
ratom
22
2
2
~
Constructive coherent
Total Cross-section by an atom (Z electrons):
Z
r
atom
j
jr
d
d
d
d
d
d
dd
d
d
S
Z
rS
atom
j
jr
Different angular distribution due to
interference
Z
r SS
atomatom
j
jr
jr
Zdd
dd
d
d
Phase relationship
The bound electron is driven by the e-field of the wave
Oscillating dipole moment results in radiation