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Electron source
Probe-forming lens
Sample (clusters)
DF-STEM detector
Aperture
HAADF-STEM detector
BF-STEM (EELS) detector
STEMimage x–y scan q
FIGURE 5.1 A schematic diagram of the operating principle of STEM, showing BF-STEM,
DF-STEM and HAADF-STEM detectors.
Gauss focus
Simple thin lens
Paraxial ray
Peripheral ray
Opticalaxis
Objective plane
Longitudinalaberration
Transverseaberration
Circle ofleast confusion
Drt
Dz
Drs
FIGURE 5.2 Ray diagram for a round lens with spherical aberration. Because of spherical aber-
ration, rays entering a round lens system away from the optical axis are refracted more strongly
than those entering closer to the optical axis.
Radius (nm)
Tem
pera
ture
(K
)
Cubic crystal
Decahedral
Icosahedral
Liquid
A
B
Quasi-molten
Quasi-molten
Decahedral
Icosahedral
Melt
Surface roughening
ROUGHFCCDECAICOS
00
200
400
600
800
1000
1200
1400
2 4 6 8 10
Nanoparticle diameter, D (nm)
Tem
pera
ture
, T (
K)
0300
400
500
600
700
800
900
1000
1100
1200
1300
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15
*
*
FIGURE 5.3 Phase diagrams of the structure of Au nanoparticles, presented in (A) by Marks in
19942 and (B) Barnard et al.49 in 2009. In (A), the dashed lines were extrapolated from the exper-
imental results shown in the solid lines. In (B), The solid lines were from the simulation whiles
the different symbols were experimental data. It is apparent that the general trend is similar in
both studies, though the actual phase boundaries are slightly different. In both cases, experimental
data were missing for nanoparticles smaller than 5nm in diameter.
Cluster size (nm)
Cluster size (nm)
0
0 0.5 1 1.5 2
0 0.5 1 1.5 2
0.2
0.4
0.6
0.8
1
B
A
C
0
0.2
0.4
0.6
0.8
1
HA
AD
F in
tens
ity (
a.u.
)H
AA
DF
inte
nsity
(a.
u.)
FIGURE 5.6 Three-dimensional atomic structure of an Au309 cluster. (A) 3D intensity profile
plot of Au309 derived from Figure 5.5A. A hard-sphere model for an Ino-decahedral structure is
shown with the electron beam (arrow) parallel to the fivefold axis. (B) Experimental intensity line
profile taken from the central atom column of the cluster to one of the corners. (C) Simulated
HAADF-STEM image (inset), obtained with a simple kinematical approach, of an Au309 cluster
with Ino-decahedral geometry. An intensity profile (solid curve) across one ridge is compared
with the result from a full dynamical multislice calculation (dashed line).8
Number of gold atoms along the column
0 2 4 6 8 10 12 14 16 18 20
AD
F in
tens
ity (
70–2
00m
rad)
Au309
Au[001]Au[111]
FIGURE 5.7 HAADF intensity as a function of number of Au atoms along the column, by mul-
tislice simulation.58
Lateral gold island size (nm)
Num
ber
of g
old
isla
nds
Coherent interface
Incoherent interface
1
5
5
0
2 3 4 5
Au
A <110>
C D
1 nm
B
E
G
F
5 Å
FIGURE 5.8 (A–E) HAADF-STEM images of Au nanoparticles on TiO2(110) arranged in the
order of projected particle size. The lattice coherency between Au nanoparticles and TiO2 sub-
strate changes according to the Au particle size. Panels (A) and (B) are coherent and (C)–(E)
are incoherent. (F) Magnified image of the epitaxial Au structure shown in (A). Here, two types
of Au sites are identified: on top of Ti–O columns and on top of O columns in the troughs of Ti-
containing columns (along the arrows). (G) A histogram of the formation of coherent or incoher-
ent interfaces as a function of Au nanoparticle lateral size.59
AWidth = 10.9 nm
Width = 4.3 nmB
1 nm
C
D W
2 nm
2h−Dh
FIGURE 5.9 Cross-sectional HAADF-STEM images of Au nanoparticles, supported on
TiO2(110), with width (A) 10.9 and (B) 4.3nm. (C) An atomistic model of Au nanoparticle on
TiO2. (D) A schematic Au nanoparticle showing measurements of nanoparticle dimensions.60
Hemisphericalclusters
Sphericalclusters
10
N1/3
500
2
4
6
8
10A
Dia
met
er (
nm
)D
iam
eter
(n
m)
Dia
met
er (
nm
)
15 20
10
N1/3
500
2
4
6
8
10B
15 20
10
N1/3
500
2
4
6
8
10C
15 20
FIGURE 5.12 Relationship between particle diameter and N1/3 for Au nanoparticles prepared by
three different methods: (A) colloidal nanoparticles, (B) nanoparticles by thermal evaporation and
(C) size-selected clusters performed in gas phase and soft-landed on the surface. Spherical cluster
approximation (the blue solid line) and hemispherical cluster approximation (the red dashed line)
are shown to allow comparison of overall particle geometry.64
Integrated HAADF intensity (a.u.)Integrated HAADF intensity (a.u.)
Num
ber
of p
artic
les
Num
ber
of p
artic
les
00
5
10
15
20
MP-Au38MP-Au38
0
5
10
15
20
D E
2 4 6 80 2 4 6
Au38
Au25
A
B
5 nm 5 nm
C
FIGURE 5.14 Weighing monolayer-protected (MP) Au38 clusters using size-selected Au clus-
ters. (A) Schematics showing that both types of clusters are co-deposited on the same TEM grid.
(B and C) Typical HAADF images of size-selected Au38 clusters and MP-Au38 clusters (with a
monomer arrowed). (D and E) Integrated HAADF intensities of MP-Au38 monomers are com-
pared with size-selected Au38 and Au25 clusters, respectively.65
A
B
C
D
FIGURE 5.15 Schematic representation of some possible atomic structures of bimetallic nano-
particles. (A) Core–shell, (B) sub-cluster segregation, (C) mixed and (D) three shells.66
Inte
nsity
Position (nm)
A B
0.0 0.2 0.4 0.6 0.8 1.0 1.2
4278
385Diameter = 4.5nm Diameter = 3.5nm
FIGURE 5.20 (A) One-dimensional HAADF-STEM (black) and EELS (red) intensity profiles
across a PdcorePtshell nanoparticle, showing that the Pt shell is two layer thick. The EELS signal
is the background-subtracted Pd core loss around 420eV. (B) Two-dimensional mapping using
HAADF-STEM (left) and Pd EELS signals (right) with 0.27nm per pixel resolution.83
B
A C
40,000
35,000
30,000
25,000
20,000
15,000
10,000
50000 10 20 30 40
60 70 80 90
70
60
50
40
3020100
50,000
45,000
40,000
35,000
30,000
25,000
20,000
15,000
10,000
5000
x
z
z
y50
FIGURE 5.21 (A) HAADF image of a RhIr cluster adsorbed on a MgO(110) surface. (B) Inten-
sity surface plot of the image in (A). (C) Three-dimensional model showing the cluster structure
determined by quantitative analysis.9