Presentation of webinar - NT-MDT

Development
Basic Principles of Advanced AFM
Modes & Applications
Dr. Stanislav Leesment,, NT-MDT
16th June 2014
Webinar Overview
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AFM Operation: main principles
Topography in Contact and Noncontact modes
Phase Imaging
High Resolution
Choice of cantilever
Spreading resistance imaging (conductive AFM/Current mapping)
Kelvin Probe Microscopy (KPM)
Piezoresponce Force Microscopy (PFM)
M
Magnetic
ti Force
F
Mi
Microscopy (MFM)
Nanolithography
Force Spectroscopy
HybriD™ Mode
Questions and Answers
AFM Operation: Main Principles
AFM: Scanning by Sample
SAMPLE SCANNING
AFM: Scanning by Tip
TIP SCANNING
Topography Imaging
Imaging.
Contact and Noncontact Modes.
Contact Mode
According the Hook’s law,
law
Force interaction between tip
and the sample is
proportional to tip bending
and the cantilever stiffness.
Stiffness for contact mode
cantilevers can vary from
0 01 to several N/m
0,01
Contact-Mode Based Modes
Noncontact (Semicontact, Tapping, AM-AFM) Mode
AFM probe,
b w=50
50 kH
kHz, k = 00.5
5 N/
N/m,
Q = 80, Rt =10 nm, A0 = 5 nm
S. Belikov et al Fall 2012 MRS Proceedings, 2013
Phase Imaging
Phase Imaging. Scan Examples.
Name: Water on Mica
Environment: Air
Tip: NSG10
Size: 10x10 um
Sample and Image Courtesy:
Reinier Oropesa-Nuñez, CEAC,
Cienfuegos, Cuba
High-Resolution Imaging in AM-AFM in Air
C18H38
Phase
PTFE
Height
18 nm
50 nm
C122H246
Height
C36H74
Phase
90 nm
C242H486
Height
C390H782
Height
CnH2n+2
C18H38 2.8 nm
C22H46 3.0 nm
C36H74 4.5 nm
C60H122 7.5 nm
C122H246 15.0 nm
C242H486 29.0 nm
C390H782 49.0 nm
C122H246
Height
135 nm
550 nm
750 nm
750 nm
4 of 35
Image Courtesy: Dr. S.
Magonov, NT
NT-MDT
MDT
Development Co.
Tip Sharpness Limitation
Z
AFM line profile
X
2
Probe tip
5
R=10
R
10
nm
R=1
nm
X axis direction
Real object (e.g.
(e g DNA molecule)
10
Probes for High Resolution
Left: high-resolution AFM phase image of poly(dG)–poly(dG)–
poly(dC) triplex DNA. The top graph shows a cross-section of
the image along the white line (at the bottom part of the image).
Right: histogram of distances between adjacent peaks on crosssections taken on many molecules (overall >200 values); the
average distance is 3.4 nm (SD = 0.9 nm)
D. Klinov, B. Dwir, E. Kapon, N. Borovok, T. Molotsky and A. Kotlyar. High-resolution atomic force microscopy of duplex
and triplex DNA molecules. Nanotechnology 18 (2007), 225102.
Cantilever Choice
Cantilever Choice
NT‐MDT AFM probes
Semicontact / noncontact
Semicontact / noncontact
Contact
(tapping)
HA_C
HA NC HA HR HA FM
HA_NC, HA_HR, HA_FM
CSG01, CSG10, CSG30
NSG01, NSG10, NSG30, NSG03
Conductive
Pt
TiN
A
Au
Magnetic
W
MFM01, MFM10
MFM LM
MFM_LM
MFM_HC
Electromagnetic Properties
Spreading Resistance Imaging (SRI)
Spreading Resistance imaging
MDMO‐PPV and PCBM Blend
Top left topography obtained in SSRM mode (-5V),
top right – current mapping, bottom right current
cross-section
cross
section profile.
profile
MDMO‐PPV and PCBM Blend
Current maps with various bias voltage,
-10
10 V
-5
5V
+1 V
+5 V
-1
1V
+10 V
Conductivity Map of OTS Sample
Topography
Current
Current contrast of
“Flowers” about 2 pA
Sample Courtesy: Prof. Jacob Sagiv, Weizmann Institute of Science, Israel
Probes for Spreading Resistance
Probes for Spreading Resistance
should normally have relatively small
spring constant 0,05 – 1 N/m contact
probes and good
p
g
conductive coating
g
(PtIr, TiN, Au)
20 nm
Kelvin Probe Force Microscopy (KPFM)
Two-Pass KPFM
KPFM on Carbon Nanotubes
3
3
2
2
1
1
Topography
SKM image
It should be noticed that SKM image reveals three kinds of nanotubes :
1)) Nanotubes with electric p
potential about 1 V,, these nanotubes have smallest diameter ((about 1.5 nm))
2) Nanotubes with electric potential about 0.5 V which have diameter about 2-3 nm
3) Thickest nanotubes which give smallest contrast in SKM and have biggest diameter (4 nm)
Charge Lithography on GaAs
Raster lithography on the GaAs substrate made with a diamond coated probe. Topography (left) and Kelvin mode (right) images. p g p y( )
( g )
g
Lithography is made by surface charging under the layer of GaAs oxide. Topography image shows nothing, when the right image made in SKM mode demonstrates areas charged positively and negatively on the neutral background. Single-Pass Electric Studies: EFM, KFM, dC/dZ, dC/dV
Working frequencies: mech ≈ 70 kHz;
elec = 3-5 kHz; 2nd Eigen mode (2E) ≈ 450kHz;
3rd Eigen (3E), etc
KFM-AMnon-res dC/dZ-AMnon-res
KFM-AMres dC/dZ-AMres – 2E, 3E
KFM-PM
KFM
PMnon-res dC/dZ
dC/dZ-PM
PMnon-res
Multi-Frequency Study of Electrical Properties
Single-Pass and Double-Pass KFM of Fluoroalkanes on Mica
C
Comparison
i
off Si
Single-Pass
l P
and
dD
Double-Pass
bl P
KFM Modes
M d
F14H20 on
mica
Probes for KPFM
FMG01/Pt
Resonance frequency ~60
60 kHz
20 nm
Piezoresponce Force Microscopy (PFM)
Piezoresponse Force Microscopy
Topography
PFM studies of TGS sample.
• Cantilevers (40 N/m) with Pt
coating were used for
measurements
• AC-sample mode with
10V@100kHz applied was used
for PFM measurements.
VPFM Amplitude
20 µm
20 µm
VPFM Phase
20 µm
Piezoresponse Force Microscopy
Block scheme of PFM
PFM: Non-Orthogonal Domains
Hi h T
High-Temperature
Molecular
M l l Ferroelectric
F
l
i Crystal
C
l off Diisopropylammonium
Dii
l
i
Bromide
B
id (DIPAB)
Amplitude, VPFM
Topography
Phase, VPFM
PFM:
60V@100kH
@
z
4 m
4 m
4 m
Amplitude, LPFM
DIPAB
Phase, LPFM
426K
b
c
DIPAB – courtesy Prof.
P f T
T. Usher
U h (UC S
San
Bernardino)
4 m
4 m
35
Probes for PFM
Probes for PFM should normally have
high spring constants 1 – 100 N/m and
coating with high conductivity (PtIr, TiN)
20 nm
Magnetic Force Microscopy (MFM)
MFM Principle
Different magnetic
domain structures of
nonhomogenious Yttrium
Iron Garnet (YIG) films.
YIG film has substantial
variation of anisotropy
field along the film
thickness
Temperature Dependency
Temperature control: -28
28...+300
+300°C
C
MFM images of the cobalt monocrystal with uniaxial
anisotropy. Phase transition occurs when temperature
increases.
Images obtained from the same area, 14x40 μm. Sample
courtesy of Prof. A.G. Pastushenkov, Tver University, Russia.
Domain Structure Transformation in External Magnetic Field
Changes of the domain structure
of Au/Co/Au ...Co/Au sandwich
structure.
t t
H = 0 Oe
H = 1000 Oe
Out-of-Plain External Magnet
H = 500 Oe
H = 1500 Oe
In-Plain External Magnet
MFM Probes
MFM_LM – low moment tips
Fig. 1.
Fig
1 Topography (left) and
Magnetic MFM (right) images of
Self-Assembled particle array
after Co/Pd thin film deposition.
deposition
Scan size 3x3 um. Sample
Courtesy - Prof. Manfred
Albrecht, Chemnitz University of
Technology, Institute of Physics
MFM_HC – high correcitivity tips
Nanolithography
Types of Nanolithography
Vector lithography
on OTS layer
Modes:
- Force
- Voltage
- Current
Methods:
- Vector
- Raster
Regimes:
g
- Constant
- Gradient
- Pulse
- Pulse Gradient
3×2 ×4 = 24 Types!
Force Lithography
Voltage and Current Lithography
Local Anodic Oxidation of Titanium film
ilm
Channel width ~20 nm
Precise Closed-Loop Control
Closed-loop OFF
Closed-loop ON
Voltage Raster Nanolithography
1 µm
2 µm
Nanomanipulation
Carbon nanotubes on silicon substrate. Manipulation
p
of nanotubes in
the specified direction (before (left), after nanomanipulations (right)).
Scan size: 2.6x2.6 µm
Probes for Nanolithography
Diamond Coated Conductive Probes (DCP Series)
- DCP01
- DCP10
- DCP20
Probes with W2C, TiO, TiN and Pt
coatings were also reported to be
successfully used in nanolitho
applications
Scanning Force Spectroscopy (SFM)
Atomic Force Spectroscopy Principle
Mechanical Properties of the Sample
Force Curves on Different Materials
PDMS60
Standard Models for AFM
PDMS8
PDMS8
Rubbery materials:
PDMS8, PDMS60 and PDMS 130
Models: Hertz, Sneddon, JKR, DMT
PDMS130
Work of Adhesion
Macro
Work of Adhesion
AFM
13.9MPa
49 J/m2
32 J/m2
1.61MPa
1.74MPa
58 J/m2
52.2 J/m2
0.74MPa
0.66MPa
47–58 J/m2
42.1 J/m2
Polymer
Material
Elastic Modulus
Macro
Elastic Modulus
AFM
PDMS-8
13.4MPa
PDMS-60
PDMS-130
Force Curves measured on PS/PBD
D
D
PS
PBD
Z
Z
Force Curves on Melanoma Life Cell
Images were obtained with use of
colloidal probe CPC_SiO2-A
HybriD Mode™
HybriD Mode™ mode: One Curve – Multiple Data
In Hybrid
y
Mode™ the tip-sample
p
p distance is modulated accordingg to the qquasiharmonic law. Thus tip enters a force interaction with the sample thousands of times per
second. Force-distance curve analysis enables maps of topographical, mechanical and
electrical properties of the sample to be extracted with high spatial resolution.
C
Commonly
l Hybrid
H b id mode
d gives
i
t
topography,
h adhesion
dh i and
d elasticity
l ti it mapping
i pictures
i t
PS-LDPE Blend
T
Topography
h
Scan Size:
3×3 µm
Adh i
Adhesion
E Modulus
M d l
Polyethylene blobs on polystyrene spheres
l t
h
E Modulus overlaid over
topography
HybriD Mode + Conductivity Mapping
+
Hybrid
y
mode™ was coupled
p with spreading
p
g resistance imaging:
g g a constant
DC voltage was applied between the sample and conductive tip. Thus while
getting a topography, adhesion and elasticity properties of the sample current
going through the circle was recorded.
Complex Study of CNT
Topograpy
Current
Stiffness
Scan size: 1×1 µm
Image Courtesy: Sergey Zayats
Sample Courtesy: Dr. Irma Kuljanishvili, Saint Louis University, Department of Physics
Living Stem Cells
Topography
Modulus Map
Post-Processing Capabilities
Revolution Cartridge
Revolution Cartridge
Innovative Revolution Head
Stiff
Soft
- safe and easy Cartridge replacement
- no system tweaking required (Plug & Play)
- high throughput operation
MFM
SKM
- Change
g methods with the same pprobes
~ 40 x less probe replacements
Revolution Cartridge
Find more information at: http://ntmdt.com/titanium
http://ntmdt com/titanium
Thank you for your attention!
All the animations used in presentation can be downloaded at:
h //
http://www.ntmdt.com/spm-principles
d
/
i i l