Negative-stiffness vibration isolators can easily support the heavy weight of a combined AFM/micro-Raman system, and isolate it from low frequency vibrations more effectively than high-performance air tables or active isolation systems. Jim McMahon reports.
The need for precise vibration isolation with scanning probe microscopy (SPM) and near-field scanning optical microscopy (NSOM) systems is becoming more critical as resolutions continue to bridge from micro to nano. Whether used in academic labs or commercial facilities, SPM and NSOM systems are susceptible to vibrations from the environment.
When measuring a very few angstroms or nanometres of displacement, an absolutely stable surface must be established for the instrument. Any vibration coupled into the mechanical structure of the instrument will cause vertical and/or horizontal noise and bring about a reduction in the ability to measure high resolution features.
Traditionally, bungee cords and high-performance air tables have been the vibration isolators most used for SPM and NSOM work. The ubiquitous passive-system air tables, adequate until a decade ago, are now being seriously challenged by the need for more refined imaging requirements. Bench top air systems provide limited isolation vertically and very little isolation horizontally. Also at a disadvantage are the active isolation systems, known as electronic force cancellation, that use electronics to sense the motion and then put in equal amounts of motion electronically to compensate and cancel out the motion.
Active systems are somewhat adequate for applications with lasers and optics, as they can start isolating as low as 0.7Hz, but because they run on electricity they can be negatively influenced by problems of electronic dysfunction and power modulations, which can interrupt scanning.
Lately, the introduction of integrated microscopy systems employing multiple microscopes is enabling more complex optical measurements, but these systems are also much heavier, and there has been little vibration isolation technology available for such heavy instrumentation. Air tables, which have been liberally used for optics applications, are not ideal for these nano-scale resolution systems because of their inability to effectively isolate vibrations below 20Hz.
But now, negative-stiffness mechanism (NSM) vibration isolation is quickly becoming the choice for SPM and NSOM systems. This includes applications using atomic force microscopy (AFM) integrated with micro-Raman spectroscopy, where negative-stiffness vibration isolation is particularly well adapted. In fact, it is the application of negative-stiffness isolation that has enabled AFMs to be truly integrated with micro-Raman into one combined system. Negative-stiffness isolators can handle the heavy weight of the combined AFM/micro-Raman system, as well as isolate the equipment from low frequency vibrations, a critical set of factors that high-performance air tables and active systems cannot achieve.
The integration of AFM with micro-Raman enables a sizable improvement in data correlation between the two techniques and expanded Raman measurement and resolution capabilities. Micro-Raman is a spectroscopic NSOM technique used in condensed matter physics and chemistry to study vibrational, rotational, and other low-frequency modes in a system. It relies on scattering of monochromatic light, usually from a laser in the visible, near infrared or near ultraviolet range. The laser light interacts with phonons or other excitations in the system, resulting in the energy of the laser photons being shifted up or down. The shift in energy gives information about the phonon modes in the system.
Scanning samples in a micro-Raman system, however, suffers from several problems. As a sample is scanned, even a very flat sample, it is hard to keep the distance of the lens to the sample constant. Thus, as one goes from pixel to pixel under the lens of a Raman, a mixture of sample and air is sampled in the voxel (volumetric picture element) that is illuminated. This causes intensity variations in the Raman that are unrelated to the chemical composition of the sample and are artifactual. This is even more pronounced with rough samples and standard methods of auto-focus are simply not accurate enough for a whole host of problems that are being investigated today.
The atomic force microscope, being a very high-resolution type of scanning probe microscope, has demonstrated resolution of fractions of a nanometer, making it one of the foremost tools for imaging, measuring and manipulating matter at the nano-scale. The information is gathered by 'feeling' the surface with a mechanical probe.
The AFM consists of a micro-scale cantilever with a sharp tip (probe) at its end that is used to scan the specimen surface. The cantilever is typically silicon or silicon nitride with a tip radius of curvature on the order of nanometers. When the tip is brought into proximity of a sample surface, forces between the tip and the sample lead to a deflection of the cantilever. Resultant characteristics, such as mechanical, electrostatic, magnetic, chemical and other forces are then measured by the AFM using, typically, a laser spot reflected from the top surface of the cantilever into an array of photodiodes.
Most systems employing AFM in concert with Raman perform separately, executing either an AFM scan or a Raman scan independently. Direct integration of Raman spectroscopy with AFM technique, however, has opened the door to significantly improved technique and sample analyses.
Micro-Raman is a micro-technique, but when AFM is added, it becomes a nano-technique. It allows the AFM structural data to be recorded online and improves the resolution of the Raman information when the nanometric feedback of the system adjusts, with unprecedented precision, the position of each pixel of the sample relative to the lens. Also the small movements of the AFM stage provide oversampling which is a well-known technique for resolution improvement.
One integrated AFM-Raman system developed by Nanonics Imaging Ltd, in association with major Raman manufacturers such as Renishaw plc, Horiba JY and others, provides simultaneous and, very importantly, on-line data from both modalities. This advantage addresses critical problems in Raman including resolution and intensity comparisons in Raman images while permitting on-line functional characterisation such as thermal conductivity, elasticity and adhesion, electrical and other properties.
The Nanonics platform can be used for structural and photonic characterisation, as well as the structural and chemical characterisation that is available with AFM and Raman integration.
For these applications, Nanonics Imaging is the innovator of AFM and NSOM systems, including dual tip/sample scanning AFM systems, the industry's first NSOM-AFM cryogenic systems, integrated Raman-AFM systems, multi-probe AFM and SEM-AFM systems. The company also holds patents to the largest range of unique nano-probes. These probes form a NanoToolKit for its unique characterisation platforms with a variety of tasks, such as for nano-photonics, plasmonics, nano-chemical imaging and even nano-chemical deposition based on its singular NanoFountainPen technology. The company is focused on full integration of AFM technology with optics, chemical imaging and other analytical tools.
The Nanonics MultiView AFM-NSOM microscope, with its free optical axis on a standard micro-Raman, now makes it possible to integrate the separate worlds of Raman and AFM/NSOM nanocharacterisation, which has led to a new era in high-resolution Raman spectroscopy.
Facilitating this integration is not only the geometry of the AFM/NSOM platform but also a new generation of AFM glass probes that have very unique characteristics - such as hollow glass probes with cantilevered nano-pippets for material deposition, probes with glass surrounding a single nano-wire in the middle for ultrasensitive electrical measurements, or dual wire glass probes for thermal conductivity and thermocouple measurements. Glass probes are ideal for Raman integration because of their transparency to laser light and no Raman background.
Underlying this integration of AFM with micro-Raman is negative-stiffness vibration isolation, developed my Minus K Technology Inc. What negative-stiffness isolators provide is unique to SPM-Raman and other NSOM systems. In particular, improved transmissibility of a negative-stiffness isolator - that is the vibrations that transmit through the isolator relative to the input floor vibrations. Transmissibility with negative-stiffness is substantially improved over air systems and over active isolation systems.
Jim McMahon writes on instrumentation technology. Nanonics Imaging Ltd is based in Jerusalem, Israel.