Scanning force microscopy (SFM), also known
as atomic force microscopy (AFM), is a surface imaging technique based on a
purely mechanical imaging process. During its development over the last 20 years
it has become a key instrument in nanoscience and nanotechnology. In AFM a very
sharp tip attached to a cantilever is brought into very close proximity to the
surface and then scanned line by line to probe the surface texture of the
Scanning force microscopy allows in-situ
measurements which do not require staining or coating of the sample as is
necessary in electron microscopy techniques. Depending on sample parameters,
contact mode or dynamic modes (e.g. IC mode) can be used to obtain high
resolution images even on very soft samples. In contact mode the tip is scanned
continuously in very close proximity across the sample. In dynamic mode tip
sample interaction can be minimized by using a vibrating cantilever. In
addition, the dynamic mode provides qualitative information about sample
parameters by observing the phase signal.
it Useful To Have a Scanning Force Microscope For Polymer Research?
AFM achieves a higher resolution compared
with the traditional microscopy techniques such as light microscopy (LM) and
confocal laser scanning microscopy (CLSM).
Electron microscopy techniques (EM) are also
often used in polymer research and AFM can be used as a complementary tool to
study such polymer preparations which are too sensitive to be studied with an
AFM sample preparation is comparably easy,
there is neither a conductive coating required, nor any sample staining. The
samples can be kept at ambient conditions, and imaging in liquid or in organic
solvents is possible, too.
Exchanging the liquid is also possible
during the experiment using a perfusion liquid cell. The temperature can be
controlled over a wide range, normally between 0 and 240 °C.
Combining different imaging techniques saves
time and leads to more reliable and meaningful scientific results. During AFM
imaging, the sample can be observed optically in both reflected light and
transmitted light. All modern contrast enhancing transmitted light techniques as
provided by inverted optical microscopes can be used together with AFM, and all
fluorescence microscopy techniques (confocal, CLSM, TIRF) and polarized light
applications are also available.
Instrumentation and Samples
All images shown in this article were
obtained with a JPK NanoWizard® AFM. The JPK Polymer
stage and the JPK LifeScience stage was used, depending on the application
and sample mounting. The Life Science stage was mounted onto a Zeiss Axiovert
200 inverted optical microscope. Cantilevers used for imaging were from
NanoWorld, Mikromasch and Appnanotech.
The samples we studied for this report were
organic compounds, both natural and synthetic examples, such as alkanes, alkane
derivatives and aromates. The compounds are of both technical and academic
interest. The molecular weight of the samples studied in this report ranges
between 300 and 130.000 g/mol.
Figure 1. Chemical formula of hexacontane, MW 843.62 g/mol.
Hexacontane belongs to the alkanes. It is a
saturated and non-branched C chain with 60 carbon atoms (Figure 1). The length
of a C-C single bond is 154 pm, the C-C-C angle is 104°. The melting point of
the compound is between 94 and 96 °C. Hexacontane is soluble in warm xylene. For
the experiment a concentration of 0.001 - 0.01 to g/L or ~ 10-5 - 10-6 mol/L is
needed. This low concentration was reached with a dilution series. 2 mg of
hexacontane were dissolved in 2 mL warm xylene (heated to 60 °C, the boiling
point of xylene ~ 140 °C). 30 ìL of this solution was diluted with 870 ìL xylene
to a concentration of 0.03 mg/mL. 30 ìL of this solution was then diluted with
870 ìL of xylene to an end concentration of 0.001 mg/mL.
A home-made spin coater (1800 rev./min) was
used for sample preparation.
Figure 2. AFM image of a preparation of hexacontane on HOPG.
The stripes represent monomolecular layers
of hexacontane, lying next to each other. The width of one stripe corresponds to
the length of the hexacontane molecule.
A piece of freshly cleaved HOPG (highly
ordered pyrolytic graphite) was used as a sample substrate. One drop of the
diluted solution was dropped onto the substrate and spun for 30 – 60 s. For a
mechanically more stable sample preparation the sample can be heated onto a
heating plate to 140 °C for about 10 min. The sample then was imaged in dynamic
mode with a NanoWorld® SSS (super sharp silicon) tip. Best images were obtained
in “soft” dynamic mode, meaning a relatively weak damping of the amplitude where
the setpoint is near the free amplitude.
Comparing the two green areas in Figure 2
shows that both of them exhibit a pattern of parallel stripes with different
orientations. The angle between the stripes in the two domains is 60°. Figure 3
shows higher resolution images within one of the striped domains. The 7.5 nm
width of the lamellae stripes corresponds with the length of an extended
Figure 3. Hexacontane, prepared on HOPG. One lamellum has a width of 7.5 nm.
(a) image size 95 x 50 nm. (b) zoom, image size 30 x 30 nm
In Figure 4 a schematic diagram shows the
arrangement of the hexacontane molecules within the lamellar structures. The
lateral self-assembly of the molecules forms the striped patterns seen by the
Figure 4. Self-assembly of hexacontane molecules on HOPG leads to lamellar
structures with 7.5 nm width.
Higher resolution can also be achieved using
AFM. Atomic lattice resolution has been achieved under ambient conditions on
some crystalline condensed matter samples such as HOPG (highly ordered pyrolytic
graphite) and mica surfaces, as shown in Figure 5.
Figure 5. Atomic lattice resolution of a mica surface. Height image. Image
size 6.6 nm x 6.6 nm, z-range 0.4 nm. NanoWizard® AFM was installed on an
optical inverted microscope.
The organic compound used in this study is
parahexaphenyl, which can be seen as coming from a bezene structure. The
conjugated polymer is poly-para-Hexaphenylene. The oligomer p-Hexaphenyl
consists of a linear chain of six benzene rings, as shown in Figure
Figure 6. Chemical structure of p-Hexaphenyl. C36H26, molecular weight 458.60
Sample preparation was done in a vacuum
sublimation process. Hexaphenylene molecules were evaporated in vacuum (10-7
mbar) at temperatures above 330 °C onto two different surfaces, a cleaved mica
surface, and a gold coated mica surface. In both cases, the samples were heated
afterwards by a focused Ar ion laser beam.
On both mica and gold the p-6P forms
nanofibers. Depending on the substrante, the arrangement of the compound leads
to very different fiber patterns. On mica surfaces p-6P exhibit needle-shaped
aggregates, as seen in Figure 7.
Figure 7. p-Hexaphenyl nanofibres prepared on clean mica. Height (left) and
amplitude (right) images. Image size 25 ìm x 25 ìm.
The height and width distribution is quite
uniform, with a typical height around 50-70 nm, and a typical width of 350 nm.
Their widths can be in the order of several hundred nanometers with heights of a
few ten nanometers and lengths of several tens to several hundreds of microns.
Areas covered by needles aligned in the same direction can reach 1
Between the needles, a huge number of small
dots can be observed. Their density decreases in the near of the
They consist of the organic material from
which the rods are grown. The forces that drive the growth are the electric
dipole fields on the mica surface. A freshly cleaved muscovite mica surface has
a surface dipole field of 107 V/cm and the p-6P molecules grow parallel to the
direction of this field.
When irradiated with UV light (360 nm) the
needles show a deep blue fluorescence at 425 nm, as can be seen in Figure 8(c).
One future application for these nanofibres may be to use them as
Figure 8. Micromanipulation on nanofibres. The AFM tip was used to scratch
nanofibres off the mica surface. The AFM images (a) height, and (b) amplitude
have a scan size of 25 ìm x 25 ìm. The scratched area had a size 10 ìm x 10 ìm.
The fluorescence image (c) has a size of 70 ìm x 70 ìm.
Since the AFM an fluorescence microscopy can
be performed simultaneously, both optical and AFM imaging can be used in-situ to
study these types of nanofibres and their optical properties.
Here the AFM tip was used to scratch the
nanofibres from a region of the mica surface, as shown in Figure 8. A cantilever
with a relatively high spring constant (40 N/m) was used as a tool for
manipulation of the sample.
Therefore a dynamic imaging mode (IC mode)
was used for imaging at low force without disturbing the fibres. The instrument
was used in contact mode for manipulation, using an applied force of 100
Preparing p-hexaphenyl on gold-coated mica
leads to a net-like pattern as shown in Figure 9. In this case, mica’s strong
dipole field is insulated by the gold cover. Gold itself does not exhibit such a
high surface dipole field. Therefore the needles form a network on the surface
and are not aligned in parallel lines.
Figure 9. p-hexaphenyl nanofibres prepared on gold-coated mica. Needles form a
net-like structure. Image size 20 ìm x 20 ìm. Height (left) and amplitude
Polystyrene-PMMA Block Copolymer
The first block-copolymers where synthesized
in the 1950s. They contain at least minimum two different "blocks" in each
individual polymer chain, where the backbone is composed of different monomers.
Their advantage compared with traditional polymers is their improved and
controllable physical properties.
The monomers of the di-blockcopolymer
polystyrene block-polymethyl-methacrylate (PS-b-PMMA) consist of linked chains
of polystyrene und PMMA, with a molecular weight of 39,000 g/mol. For AFM
imaging this sample was prepared in a spin-coating process on a silicon
substrate. In the height image in Figure 10, the cylinders (width 10-15 nm,
height 1 nm) lying on a flat surface are clearly resolved. The rods are lying in
parallel but curved lines, and each rod can be up to several micrometers
In this case, the flat cylinders consisting
of PMMA are lying in a polystyrene matrix. In the phase image of Figure 10, the
contrast between the PMMA rods (black) and the polystyrene matrix (green) is
more clearly resolved.
Figure 10. PS-b-PMMA block copolymer. Image size 1 x 1 ìm. Height (left) and
Styrene-Butadiene-Styrene Triblock Copolymer
A well-known tri-block copolymer is SBS
(styrene butadiene-stryrene). SBS belongs to the group of thermoplastic
elastomers and is made by anionic polymerisation. In the SBS case one starts
with the anionic polymerization of styrene, and adds butadiene, after all
styrene monomers have been reacted. Starting the reaction leads to a negatively
charged ion. These reaction solutions are called “living polymers” because in an
environment free of water and protic solvents negatively charged organic ions
remain there, also after all monomers are polymerized.
Figure 11. (a) Very simple schematic view of the SBS block copolymer molecule.
(b) Chemical structure of the polystyrene and polybutadiene sections. Parts
formed from styrene monomers (red) and butadiene monomers (blue) are
Pure polystyrene is a brittle and tough hard
plastic, and this gives SBS its durability. Polybutadiene is rubbery, and this
gives SBS its rubber-like properties and prevents the polystyrene from breaking.
During the reaction the lengths of the styrene or butadiene chains can be
controlled individually. Copolymers with a short soft butadiene-chain are highly
transparent, shiny and impact resistant. The polymer is used for food and
cosmetics packaging and shrinking foil, those with longer butadiene chains for
shoe soles and tire treads. The molecular weight of the sample used here was
Figure 12. SBS block-copolymer imaged in IC mode. Image size 1 ìm x 1 ìm. Left:
height image, right: phase image. In the phase image dark areas correspond to
polybutadiene, bright areas to polystyrene.
For AFM measurements SBS had to be prepared
on a solid support. First, SBS was dissolved in toluene to a final solution of 5
% w/v. The thin films supported by a glass cover slip were prepared on a spin
coater (1800 rev./min).
Vacuum annealing of SBS at temperatures
above 100 °C (190 °C in this case) leads to nano-phase separation. In contrast
to the AFM height images of PS-b-PMMA (Figure 10), the height image in Figure 12
exhibits a relatively featureless surface, with pits of 80 nm in diameter and 3
- 4 nm in depth. The phase image exhibits a strong contrast from 10-15 nm wide
dark rods in a bright matrix, where the rods are 60 nm or longer. The histogram
analysis of the phase image in Figure 13 (a) clearly resolves the two
In this case the sample is a styrene-rich
SBS. Some block copolymers show de-mixing phenomena due to the insolubility of
polybutadiene in polystyrene. From transmission-electron-microscopy (TEM) data
it is known that butadiene forms hexagonally packed cylinders, embedded in a
styrene matrix, as shown schematically in Figure 13. This means that in the
phase image of Figure 12, the dark areas correspond to polybutadiene and bright
areas to polystyrene.
Figure 13. (a) Histogram of the values in the phase image of Figure 12. (b) In
a styrene-rich SBS the minority phase (polybutadiene) forms a hexagonally
close-packed cylinder structure.
Like the copolymers also biaxially-oriented
polypropylene (BOPP, a newer abbreviation is PP-BO) belongs to the polymers that
are common in everyday use. The name comes from the manufacturing process in
which a polypropylene foil is stretched in two directions. The AFM image in
Figure 14 reveals a fiber-like structure. Fibres are not completely separate and
are oriented from the upper left to the bottom right side of the image.
Connecting fibres also can be seen spreading from left to right.
Figure 14. Biaxially-oriented polypropylene foil. Image size 800 nm x 800 nm,
height range 33 nm. Height (left) and phase (right) images.
Compared with standard polypropylene foils
PP-BO has got an increased transparency and brilliance but also added better
mechanical parameters such as added tear and scratching resistance as well as a
high stiffness, a good low temperature resistance and impermeability for liquids
and gases. PP-BO is widely spread, also for household use (bags, foils).
Monoaxially-oriented polypropylene which is only stretched in one direction is
often used for adhesive foils. Since 10 years, an increasing number of countries
others) issue their banknotes made out of PP-BO due to their wear resistance and
higher number of options to add security features.
Some bacteria use poly-hydroxybutyrate (PHB)
as a food storage molecule. By changing the feedstock they can also be forced to
produce a copolymer named PHB-PHV consisting of
poly-hydroxybutyrate-poly-hydroxyvalerate that contains ù-hydroxy valeric acid
Figure 15. Chemical formula of poly-hydroxybutyrate. It is synthesized in a
polycondensation reaction of ù-hydroxy butyric acid monomers.
Many polymers tend to fold along the chain
length to form large flat crystals, with a thickness much smaller than the
lateral dimensions. These lamellae are often formed parallel to each other and
form layered crystal sheets. The sheets also can form larger arrangements, where
the lamellae grow approximately radially out from the center of a polymer
spherulite. The images displayed in Figure 16 show the central section of one
these spherulite structures.
Figure 16. Height image (left) and phase image (right) of a spherulite
structure in a PHB-PHV film. Image size 8 ìm x 8 ìm, height range 140
Assembled Monolayers of Phosphonic Acid with Long Alkyl Chain
Octadecylphosphonic acid (OPA) is an
amphiphilic molecule with a C-18 alkyl chain and a phosphonic acid group on one
end (Figure 17). It is used for modification of oxidic metal surfaces
(passivation). On aluminum surfaces it serves as a corrosion protector and it
has also been used for chemical modification of titanium implant
Figure 17. Octadecylphosphonic acid (OPA), CH3(CH2)17PO3H2,
molecular weight 334,5 g/mol.
Preparing OPA on mica leads to robust
self-assembled monolayers. For the preparation of OPA monolayers on mica, OPA is
dissolved in ethanol (0.25 mM) and the solution is spread onto a freshly cleaved
sheet of mica (8 x 8 mm). The OPA is allowed to adsorb for 10 s, then the excess
solution is removed with a stream of dry nitrogen.
Figure 18. OPA prepared on mica leads to monomolecular layers. Scan size 2 x 2
ìm. Height (a), error (b) and lateral force (c) images.
AFM imaging was performed in contact mode
with a very soft cantilever (spring constand 40 mN/m) for lateral force mode. In
the height images small round dots with diameters in the 100 nm range are
clearly resolved. But also larger curvilinear plaques with diameters up to 1 ìm
can be observed. The cross section displayed in Figure 19 indicates that the
average height step is 2.3 nm. The histogram analysis of the height image also
shows this uniform height distribution. The height of the plaques corresponds
with the length of a single OPA molecule.
Figure 19. (a) The cross-section indicates the height of the OPA monolayer. (b)
Histogram analysis of the OPA height image. Two peaks are clearly
In the lateral force image in Figure 18 (c),
the plaques indicate a relatively low lateral deflection and thus a lower
friction compared with the friction on the pure mica surface.
On the areas uncovered by OPA a pattern of
brighter and darker domains is resolved which is invisible in the vertical
In this report we presented AFM-based
studies on samples made from alkanes, alkane derivatives, aromates and polymers.
Information about the sample surface properties could be obtained on a
micrometer and a nanometer range. Molecule assemblies could be resolved up to
the length of single molecules. Phase separation phenomena also could be
studied, not only depending on the pure surface properties alone. In case of
fluorescent samples we successfully combined fluorescence microscopy with
We thank Dr. Fank Balzer,
Humboldt University Berlin, Germany for the
para-hexaphenyl nanofibre samples, Prof. Thomas Thurn-Albrecht,
University of Halle, Germany, for the
PS-b-PMMA sample, Dr. Heng-Yong Nie, London, Ontario,
Canada for the BOPP foil
and Prof. Mervyn Miles, Bristol
University, England, for
the spherulite sample.