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FlexAFM

Atomic force microscope
팁을 사용하여 표면 형상 측정 및 표면 분석

ico_chk01  도립 현미경과 호환 가능하여 현미경으로 targeting 후 바로 AFM 측정 가능 (호환 가능 현미경 : Zeiss, Nikon, Olympus, Leica )

 

ico_chk01  다양한 옵션과 사용 중 옵션 추가 가능 (sample heating stage, environmental control option 등)

 

ico_chk01  Lateral Force Microscopy, Kelvin Probe Force Microscopy, C-AFM, Scanning Thermal Microscopy 및 Fluid Force Microscopy 등의 고급 옵션 활용 가능

 

ico_chk01  Air 또는 Liquid 상태 시료 측정 가능

 

ico_chk01  현미경 하에서 보이는 sample을 대상으로 매우 정확한 압력과 힘으로 제어 가능

 

ico_chk01  나노미터 스케일의 AFM

Versatility and performance for biology and life science

For success in life science research, scientists depend on professional tools that can readily provide the information needed, regardless of the tasks at hand. By combining key technologies and components, Nanosurf has made the FlexAFM system one of the most versatile and flexible AFM systems ever, allowing a large variety of biological and life science applications to be handled with ease. With the FlexAFM, you can combine the liquid AFM imaging, spectroscopy and nanomanipulation capacity of this system with the high-end optical techniques available for inverted microscopes.

FlexAFM

Flexible system design for life science research

FlexAFM comes with manual and motorized stages for seamless integration on Zeiss, Olympus, Nikon and Leica inverted microscopes or with standalone stages. On the inverted microscope, optical and AFM data can be correlated, as shown here for internal limiting membrane (ILM) of the human retina.

combined imaging

(A) Bright field image of isolated ILM in a physiological buffer. (B) Fluorescence image of the same section showing anti-laminin staining. (C) AFM topograph of a subsection of the ILM; also shown as overlay in B. (D) AFM stiffness measurements (stiffness map) of the same subsection. The color for each point represents the local stiffness value as calculated from force curves recorded at the respective positions. (E) Histogram of the stiffness data shown in D. (F) Typical force-displacement curves obtained on the ILM and on the glass substrate. These curves are converted to force-indentation data, which then allows calculation of the stiffness. Stiffness distribution of biological tissues has been shown to be a marker for diseases such as age-related macular degeneration, arthritis and cancer. Data courtesy: Marko Loparic, Marija Plodinec, Philip Oertle, and Paul B. Henrich, Biozentrum/SNI/UHBS, University of Basel, CH.

The modular stage, cantilever holder, and software concept allows an easy upgrade of the system to access many new possibilities in life science and materials research. Flex-FPM for cell and nano-manipulation, for example, and Flex-ANA for automatic nanomechanical analysis. In addition, advanced modes like MFM and KPFM that were originally developed for the Flex-Axiom system, are also available for FlexAFM. For measurements that don’t need optical access from below, e.g. for the imaging and spectroscopy of samples like bacteriorhodopsin, a standalone stage makes the FlexAFM compatible with the Nanosurf Isostage and Acoustic Enclosure 300, and generally makes the system much more compact.

Flex-Bio system with stage

A FlexAFM system with stand-alone stage, isostage, and acoustic enclosure. (B) 2D crystals of bacteriorhodopsin [140 nm scan range]. (C) Power spectrum of B, showing a lateral resolution of well over 1 nm [dashed circle]. (D) Single molecule force spectroscopy of bacteriorhodopsin.

FlexAFM lifescience application examples

Imaging of type I collagen fibrils

Collagen is the most abundant protein in mammals and contributes to more than 25% of the whole-body protein content. It is the main structural protein of the extracellular matrix of connective tissues and provides e.g. tendons and bone with their tensile strength. Most of the collagen found in mammals is fibrillar type I collagen. Type I collagen fibrils show a typical periodic morphology, the so-called D-banding. D-bands result from staggered self-assembly of individual collagen molecules into larger fibrils with a periodicity of about 67 nm. Images of collagen fibrils from rat tendon were recorded in Prof. Snedeker’s research group at the ETH Zürich. One of the reasearch areas of Prof. Snedeker is tendon mechanics and biology.

3D AFM topography of several type I collagen fibrils

3D AFM topography of several type I collagen fibrils

AFM topography image of collagen

AFM topography image of type I collagen fibrils

AFM deflection image recorded along with the topography image

AFM deflection image recorded along with the topography image

The 3D representation of the AFM topography image nicely shows the typical periodic D-banding of type I collagen on all fibrils. The colloagen topography was recorded in static mode using a Nanosensors PPP-XYCONTR cantilever. AFM images were processed using Nanosurf Report Software. Preparation and imaging of collagen fibrils was performed by Massimo Bagnani, Prof. Snedeker research group, Uniklinik Balgrist, Institute for Biomechanics, ETH Zürich, Switzerland.

Measurements on living cultured cells

Mechanobiology is an emerging research area that deals with the effect of changing physical forces or changes in the mechanical properties of cells and tissues. Several diseases, such as fibrosis and atherosclerosis are associated with changes in tissue stiffness. Moreover, in cancer, the metastatic potential of cancer cells depends on their elastic modulus. Here, the elastic modulus of living cells from a human breast basal epithelial cell line was measured using a Nanosurf FlexAFM system with the Flex-ANA software.

Elastic modulus map

Elastic modulus map

Unperturbed cell topography

Unperturbed cell topography from force mapping

The first image shows the elastic modulus (in kPa) recorded on living breast epithelial cells immersed in cell culture medium. Differences in the elastic modulus within the cell can be clearly observed. The dark area surrounding the cells originate from the much stiffer cell culture dish substrate. The second image shows the unperturbed cell topography extracted from the force mapping data. The topography is determined from the contact point of each force curve and thus shows the cell topography at zero applied force.

Elastic modulus mapped to the 3D topography

Elastic modulus mapped to the 3D topography

Elstic modulus distribution

Elstic modulus distribution

Mapping the elastic modulus data to the 3D topography allows relating the information of both channels. The 3D image was generated using Gwyddion software. The last image shows the distribution of the elastic moduli extracted from nanomechanical force mapping experiments. The peak at lower moduli corresponds to the stiffness of the cells. The peak at the right originates from the cell culture substrate and shows much higher elastic moduli. AFM data courtesy of Philipp Oertle, Biozentrum, University Basel.

Single molecule force spectroscopy of bacteriorhodopsin

The force-distance curve below reports the controlled C-terminal unfolding of a single bacteriorhodopsin (BR) membrane protein from its native environment, the purple membrane from Halobacterium salinarium. Solid and dashed orange lines represent the WLC curves corresponding to the major and minor unfolding peaks observed upon unfolding BR, respectively. The contour length of the stretched polypeptides of the major unfolding peaks is given in amino acids (aa).

single molecule force spectroscopy

Single molecule force spectroscopy of bacteriorhodopsin

This data was recorded using a FlexAFM scan head (10-µm; version 3) in combination with the C3000 controller and a cantilever with a nominal spring constant of 0.1 N/m (Uniqprobe, qp-CONT, Nanosensors).

FlexAFM image gallery

Cell-cell adhesion force studied with Flex-FPM
Cell-cell adhesion force studied with Flex-FPM
Nanomechanical analysis of alginate hydrogels
Nanomechanical analysis of alginate hydrogels
AFM imaging of type I collagen fibrils
AFM imaging of type I collagen fibrils
AFM topography of a living HeLa cell
AFM topography of a living HeLa cell
High resolution imaging of the cytoplasmic side of bacteriorhodopsin
High resolution imaging of the cytoplasmic side of bacteriorhodopsin
Living Rat-2 cells
Living Rat-2 cells
Imaging DNA with the AFM
Imaging DNA with the AFM
Tissue samples
Tissue samples
Dynamic mode AFM of human hair
Dynamic mode AFM of human hair
AFM for dental implants
AFM for dental implants
AFM image of butterfly wings
AFM image of butterfly wings

The most flexible atomic force microscope for materials research

For success in materials research studies, scientists depend on professional tools that can readily provide the information needed, regardless of the tasks at hand. By advancing key technologies and designs, Nanosurf has made the FlexAFM one of the most versatile and flexible AFMs ever, allowing a large variety of materials research applications to be handled with ease. In combination with the powerful C3000i controller, complex material characterizations are possible.
Flex-Axiom

The precision and performance you need for your research

The FlexAFM uses an extremely linear electromagnetic scanner for XY movement. This scanner delivers an average linearity deviation of less than 0.1% over the full scan range, top-ranking on the AFM market. The Z-axis is piezo-driven, with a position sensor that enables closed-loop operation. A sensitive cantilever detection system can measure well into the MHz frequency range. The scan head is connected to the full-featured, 24-bit C3000i controller with digital feedback and 2 dual-channel lock-in amplifiers.

Imaging of single and multiple pyrene nanosheets and height analysis with sub-nanometer accuracy

Imaging of single and multiple pyrene nanosheets and height analysis with sub-nanometer accuracy. Data courtesy: Mykhailo Vybornyi, University of Berne, Switzerland

Topography of SrTiO3 in dynamic mode

Strontium titanate (SrTiO3, STO) is an oxide of titanium and strontium exhibiting a perovskite structure. It has interesting and partly unique material properties. It is used as substrate for growth of oxide-based thin films and high-temperature superconductors. STO forms surfaces that show a layered structure. The thickness of individual layers is in the range of a few Angstrom. Atomic force microscopy is an ideal tool to image and measure these structures.

AFM topography showing steps of strontium titanate

Topography showing steps of strontium titanate; image size 1.1µm

Section profile and height distribution

Section profile and height distribution

The sample clearly shows the typical layer structure STO. Here, the layers are not perfectly smooth, but exhibit residual roughness of approx. 125 pm (RMS). This is caused by a non-ideal termination process during the preparation of this STO sample. The graph shows the profile of the image shown above along a line extending from the top left to the bottom right corner of the imaged area. The profile also clearly shows the layered structure of the sample and reveals step heights of approx. 4 Å. Similarly in the right panel, the height distribution histogram of the image above clearly shows approx. 4 Å-spaced peaks for the different layers of the sample.

Topography and KPFM of CVD grown molybdenum disulfide monolayers

In this application note, monolayer MoS2 grown by chemical vapor deposition (CVD) was imaged with Kelvin probe force microscopy (KPFM) using a FlexAFM to study the contact potential difference variation on a single crystal. Monolayers of MoS2 were grown on a silicon substrate by chemical vapor deposition (Sample courtesy: University of Illinois – Urbana-Champlain). Non-uniformity of the contact potential signal across the monolayer can inform about doping profiles and other surface defects.

MoS2 optical micrograph

MoS2 monolayers optical micrograph

AFM topography MoS2 monolayer

a) AFM topography image of single MoS2 monolayer. Location where profile is taken indicted by red line. b) Height (top) and KPFM voltage (bottom) profile across monolayer

Measurements using the FlexAFM show a step height of 0.6 nm for the MoS2 monolayer. Concurrent KPFM measurements show a 650 mV contact potential difference between the monolayer and the SiO2 substrate.

3D AFM topography overlay MoS2

3D AFM topography overlay MoS2

All measurements were performed using a FlexAFM system equipped with a ANSCM-PA cantilever from AppNano. Images were processed using MountainsMap SPM. For more information contact our application scientists

KPFM and MFM on stainless steel

In the experiment shown below, KPFM and topography data were recorded in a single run using a FlexAFM system. Also see the related MFM application.

KPFM on stainless steel

KPFM overlay on a topography image of stainless steel Scan size: 80 µm x 80 µm Potential range: 200 mV

Topography on stainless steel

The topography image itself Scan size: 80 µm x 80 µm Height range: 50 nm

MFM zoom on stainless steel

MFM image of the same area Scan size: 80 µm x 80 µm Phase range: 10°

FlexAFM image gallery

Magnetic force microscopy of thin permalloy film with stripe domains
Magnetic force microscopy of thin permalloy film with stripe domains
Topography of SrTiO3 in dynamic mode
Topography of SrTiO3 in dynamic mode
 Magnetic force microscopy of digital backup tape
Magnetic force microscopy of digital backup tape
Topography on multilayer graphene
Topography on multilayer graphene
KPFM on multilayer graphene
KPFM on multilayer graphene
Topography of MoS2 monolayer
Topography of MoS2 monolayer
MoS2 monolayer: 3D topography overlaid with KPFM signal
MoS2 monolayer: 3D topography overlaid with KPFM signal
Topography of locally deposited charges on an insulating oxide surface
Topography of locally deposited charges on an insulating oxide surface
KPFM of locally deposited charges on an insulating oxide surface
KPFM of locally deposited charges on an insulating oxide surface
Topography of an integrated circuit structure with multiple transistor contacts
Topography of an integrated circuit structure with multiple transistor contacts
Conductive AFM of an integrated circuit structure with multiple transistor contacts
Conductive AFM of an integrated circuit structure with multiple transistor contacts
Out of plane PFM on Lithium Niobate
Out of plane PFM on Lithium Niobate
Electrostatic force (EFM) measurements on aluminum dots deposited on gold
Electrostatic force (EFM) measurements on aluminum dots deposited on gold
Topography of polished stainless steel
Topography of polished stainless steel
Magnetic force microscopy on polished stainless steel
Magnetic force microscopy on polished stainless steel
KPFM on polished stainless steel
KPFM on polished stainless steel
Nanomechanical analysis of alginate hydrogels
Nanomechanical analysis of alginate hydrogels
Electrochemical AFM with rod-like samples: Cu deposition on a commercial Pt electrode
Electrochemical AFM with rod-like samples: Cu deposition on a commercial Pt electrode
Dynamic mode AFM of pyrene nanosheets
Dynamic mode AFM of pyrene nanosheets
Dynamic mode AFM of polished sapphire
Dynamic mode AFM of polished sapphire
AFM force spectroscopy on a polymer blend
AFM force spectroscopy on a polymer blend
AFM phase image of a polymer blend
AFM phase image of a polymer blend
Topography analysis of ePTFE membrane using AFM
Topography analysis of ePTFE membrane using AFM
Airplane Wing Coating
Airplane Wing Coating
Topography of solar cell layers
Topography of solar cell layers
Screw dislocations in GaN
Screw dislocations in GaN
Dynamic mode AFM on pentacene film on TiO2
Dynamic mode AFM on pentacene film on TiO2
Morphology analysis of paper
Morphology analysis of paper
Contact mode AFM of polished ceramic plate used in dentistry
Contact mode AFM of polished ceramic plate used in dentistry
MFM of bits on a harddisk
MFM of bits on a harddisk
AFM for dental implants
AFM for dental implants
Static force AFM of stainless steel
Static force AFM of stainless steel
FlexAFM 5 scan head specifications with C3000i controller 100-µm scan head 10-µm scan head
Sample size Unlimited without sample stage 100 mm on sample stage
Maximum Petri dish height (fluid level) 9 mm (6 mm)
Manual height adjustment range 6 mm
Motorized approach range (at tip position) 2 mm
Max. scan range (XY) 100 µm1 10 µm1
Max. height range (Z) 10 µm2 3 µm1
XY-linearity mean error < 0.1%
XY-flatness at maximum scan range typ. 5 nm typ. 1 nm
Detector bandwidth DC – 4 MHz
Detector noise level (RMS) typ. 60 pm / max. 100 pm (3, 4)
Z-sensor noise level (RMS) typ. 180 pm / max. 200 pm (3)
Z-measurement noise level (RMS, static mode in air) typ. 100 pm / max. 200 pm
Z-measurement noise level (RMS, dynamic mode in air) typ. 35 pm / max. 50 pm
Scan head dimensions 413 x 158 x 53 mm
Scan head weight 1.25 kg
(1) Manufacturing tolerances ± 5%

(2) Manufacturing tolerances ± 10%

(3) Measured at 2 kHz

(4) Measured with XYContr cantilever