Scanning Thermal Microscopy
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With the development of the easyScan 2 FlexAFM, Nanosurf offers a platform with increased flexibility for researchers that require advanced imaging modes, while still maintaining Nanosurf's trademark ease of use. Experiments that were not possible with the previous easyScan systems are now routine with the FlexAFM. Being able to accommodate a much greater selection of specialty cantilevers while providing easy access to system inputs and outputs is one of the many advantages that the FlexAFM offers. This advantage is demonstrated with the integration of Scanning Thermal Microscopy (SThM) imaging and local thermal analysis capabilities that are offered by Anasys Instruments.
Figure 1. Scanning Electron Microscopy (SEM) images of an Anasys thermal probe. (Left) Entire cantilever. (Right) Magnification of the tip.
Scanning Thermal Microscopy
Scanning Thermal Microscopy is an AFM imaging mode that maps changes in thermal conductivity across a sample's surface. Similar to other modes that measure material properties (LFM, MFM, EFM, etc.), SThM data is acquired simultaneously with Topographic data. The SThM mode is made possible by replacing the standard contact mode cantilever with a nanofabricated thermal probe with a resistive element near the apex of the probe tip.
This resistor is incorporated into one leg of a Wheatstone bridge circuit, which allows the system to monitor resistance. This resistance correlates with temperature at the end of the probe, and the Wheatstone bridge may be configured to either monitor the temperature of a sample or to qualitatively map the thermal conductivity of the sample. Changes in sample temperatures are often measured on active device structures.
For example, it is possible to image hot spots and temperature gradients on devices such as magnetic recording heads, laser diodes, and electrical circuits. Thermal conductivity imaging, however, is commonly applied to composite or blended samples. In this mode, a voltage is applied to the probe and a feedback loop is used to keep the probe at a constant temperature.
As the thermal probe is scanned across the sample surface, more or less energy will be drained from the tip as it scans across different materials. If the region is one of high thermal conductivity, more energy will flow away from the tip. When this occurs, the thermal feedback loop will adjust the voltage to the probe to keep it at a constant temperature. When the probe moves to an area of lower thermal conductivity, the feedback loop will lower the voltage to the probe, as it will require less energy to keep the probe at a constant temperature. By adjusting the voltage to keep the probe temperature constant, a map of the sample's thermal conductivity is generated.
Figure 2: Imaging of a carbon fiber and epoxy sample. (Top) Topography image. Z-range corresponds to 1.4 µm. (Bottom) SThM image. Z-range corresponds to 600 mV. The XY-range of both images corresponds to 80 µm x 90 µm.
Figure 2 displays simultaneously acquired Static Mode Topography and SThM images of a carbon fiber and epoxy sample. The sample has been cross-sectioned and polished to provide a flat surface. Having a smooth surface will minimize changes in the SThM contrast that result from topographic effects. In the SThM image here, it is possible to map the thermal conductivity difference of the epoxy regions and the carbon fibers. As expected, the carbon fibers are seen to have a higher thermal conductivity (light blue) than the surrounding epoxy regions (purple). These data also serve to verify the sub-100-nm resolution that is expected from the thermal probes.
Beyond adding the extended capabilities of SThM imaging, it is also possible to acquire local quantitative thermo-mechanical information with sub-100-nm resolution. This is possible with the nano-TA option offered by Anasys Instruments. Once an area of thermal interest has been identified using standard Topography imaging with the thermal probe, it is then possible to place the probe at a specific point to measure local thermal properties.
This information is obtained by linearly ramping the temperature of the nano-TA probe with time while monitoring deflection of the probe. The thermo-mechanical response allows the user to obtain quantitative measurements of phase transition temperatures such as melting point (Tm) and glass transition temperatures (Tg). At the point of these phase transition temperatures, the sample beneath the probe will soften, allowing the probe to penetrate into the sample. As seen in Figure 3, this produces a plot of probe deflection as a function of temperature. This breakthrough in spatial resolution of thermal properties has significant implications in the fields of Polymer Science and Pharmaceuticals where understanding local thermal behavior is crucial.
Figure 3. Local nano-TA analysis of a poly-ethylene film. Graph showing measurement results that were performed at two individual sample sites (blue and red curves, respectively). The onset of melting occurs at 115°C.
The easyScan FlexAFM with Signal Module A and Cantilever Holder ST is required to perform SThM imaging and/or local nano-TA sample analysis (see Figure 4). Anasys Instruments provides hardware and software that easily integrate with the FlexAFM system.
Figure 4. Nanosurf components required for SThM measurement. (Top) The Nanosurf easyScan 2 FlexAFM scan head. (Bottom left) The easyScan 2 Signal Module A. (Bottom right) The FlexAFM Cantilever Holder ST.
Anasys thermal probes are premounted on supports (Figure 5, top) that are compatible with the FlexAFM Cantilever Holder ST. In the experiments described here, the Anasys GLA-1 and AN2-200 thermal probes were used. The Anasys SThM system (Figure 5, bottom) includes a simple software interface that controls the thermal analysis electronics via a USB connection. This interface is capable of outputting a low-noise, high-resolution voltage to the probe.
Figure 5. Anasys components required for SThM measurement with the FlexAFM scan head. (Top) Anasys thermal probes. (Bottom) Anasys SThM electronics comprising the power supply, controller, and CAL box.
The voltage may be varied over a wide range depending on the probe type and the desired temperature of the probe (<0.1°C resolution). The other components in the bridge circuit are easily changed if required for custom experiments, and the system includes an input connection to apply AC voltages to the probe. The resistance of the probe is output on a BNC, which is then connected to User Input 1 on the easyScan 2 Signal Module A. For SThM imaging, the easyScan 2 control software is configured to collect the resistance data on User Input 1, allowing SThM information to be recorded and displayed as a chart in the imaging window of the Nanosurf software. During nano-TA experiments, the Anasys software allows the User to set Nano-TA2 controller parameters such as heating rates and temperature range. Typically, AFM feedback is turned off during the acquisition of nano-TA data.
This information has been sourced, reviewed and adapted from materials provided by Nanosurf AG.
For more information on this source, please visit Nanosurf AG.