This invention relates to an atomic force microscope (AFM) tip holder and more particularly to an AFM tip holder for imaging in liquid.
Atomic force microscopes reveal the microscopic structure of a variety of materials to the nanometer. This tool has become essential for characterizing the surface of numerous materials including biological materials.
Biological material samples such as DNA, living cells, and proteins must remain immersed in liquid (reproducing the sample's normal physiological conditions) during imaging in order for the sample to live and retain its inherent biological characteristics. Most often a tapping mode technique is used to image biological samples in liquid in order to prevent significant damage to the sample which is soft and fragile. Ando et al., “A high-speed atomic force microscope for studying biological macromolecules,” PNAS, Oct. 23, 2001 (Vol. 98, No. 22), (incorporated herein by reference) describe the “tapping mode” AFM imaging of molecules. Hallett et al., in “Improvements in atomic force microscopy protocols for imaging fibrous proteins,” J. Vac. Sci. Technol. March/April 1996 (p. 1444) (incorporated herein by reference), describe tapping mode AFM imaging of proteins in liquid. In tapping mode, an AFM cantilever is positioned above the surface of a sample and oscillated at its natural resonant frequency by means of a piezoelectric stack so that a cantilever tip taps the surface of the sample only for a small fraction of the oscillation period. The tip-sample interaction is measured through changes in the amplitude, phase, and/or resonant frequency of the oscillation. This tip-sample interaction is mapped into the surface topography of the sample through any of several AFM detector means well known in the art and not a part of the invention here.
Current AFM technique imaging biological specimens in liquid uses a generally similar design in which the tip scanning the specimen is fully submerged in the liquid. Sulchek et al., “High-speed atomic force microscopy in liquid,” Review of Scientific Instruments, May 2000 (Vol. 71, No. 5) (incorporated herein by reference) describe shortcomings of AFM scanning in liquid as compared to air.
Liquids are more viscous than air, and therefore, create more drag on the cantilever and cantilever tip as they oscillate in the liquid. This impacts the imaging process in several negative ways. The cantilever moves more slowly, or at a decreased frequency. The movement of the cantilever in liquid causes significant background “noise” in the tip-sample interaction measurements and makes it harder to determine the natural resonant frequency of the cantilever. These in turn affect the accuracy and resolution of the resulting surface image.
When the tip and supporting cantilever oscillates in the more viscous liquid medium (i) a large volume of the liquid is disturbed, (ii) the resonant peak is widened greatly complicating lateral resolution in the imaging, and (iii) desired faster scanning is complicated or prevented by the slowing of the cantilever and tip and the further difficulties of AFM scanning in liquid.
A further problem in liquid imaging is commonly referred to as the “forest of peaks.” When the cantilever and tip oscillate in liquid, the viscous liquid causes mechanical resonance in the cantilever and tip itself, which in turn introduces numerous sharp peaks in a cantilever's response spectrum (graph of amplitude versus frequency). The “forest of peaks” introduced into the response spectrum masks the major peak that corresponds to the cantilever's natural resonant frequency.
The present invention is an AFM tip holder for imaging in liquid using the well-known phenomenon of excluding liquid from an open bottom sealed vessel when it is immersed into the liquid well below the liquid level.
The present invention is an apparatus that maintains most of an AFM's cantilever tip and the entire cantilever in air (or other environmental gas), rather than in the more viscous liquid. This thereby reduces and/or virtually eliminates the negative effects discussed above, leading to higher-resolution images of samples in liquid. Specifically, with most of the cantilever tip and cantilever moving through less viscous air or gas, a higher drive frequency can be used in imaging as much as three to five times that in liquid. A high drive frequency allows for faster scanning which in turn can allow for study of the dynamic behavior of biological materials (“fast-scanning AFM”). A narrow resonant peak very close to that accomplished scanning in air can be expected.
Importantly, maintaining most of the cantilever and cantilever tip in air as it oscillates eliminates the “forest of peaks,” making the one major peak corresponding to the cantilever's natural resonant frequency easily identifiable. Oscillating the cantilever and tip in air rather than liquid typically increases the accuracy of the natural resonant frequency determination by a factor of 10. Accurate identification of the cantilever's natural resonant frequency is important because oscillation at the natural resonant frequency allows for high-resolution imaging of the sample surface and faster imaging.
The present tip holder invention can also be used for active cantilevers operating in air without any modification, which may further lend to the development of faster AFM scanning of biological subjects in liquid. This can be important because biological specimens such as live cells can rapidly change. Also, when using the tip holder of the present invention, if the level of the liquid in which a specimen is retained varies considerably, very little variation of the liquid level at the scanning tip occurs.
The above and further objects and advantages of the invention will be better understood from the following detailed description of at least one preferred embodiment of the invention, taken in consideration with the accompanying drawing.
Referring to
When the tip holder 14 is immersed into the liquid 24 in which a biological sample rests, the liquid level 21 within the tip holder raises up at a value considerably less than the liquid level 30 outside the tip holder. Put another way, partial immersion of the tip holder 14 depresses the liquid surface at the level 21 allowing it to rise within the holder 14 only an amount permitted, by the compression of the air or other contained gas. It is estimated that if an air-filled tip holder 14 is immersed 2 millimeters into the liquid, the level of the liquid inside the tip holder raises less than 1 micrometer. This is only one-tenth of the cantilever tip height if the height of the pyramidal or conical cantilever tip 20 is 10 micrometers. The level raises another 2 micrometers if the tip holder 14 is moved down an additional 3 millimeters into the liquid (5 millimeters total). If the bottom of the cantilever tip 20 is exactly even with the lower rim 22 of the vessel 19, the major part of the cantilever tip 20 remains above the liquid level 21 and the entire cantilever 10 resides above the liquid and does not touch the liquid while the scanning is performed.
Whereas a specific, preferred exemplary embodiment of the invention has been described above, it will be apparent to those skilled in the art to which the invention pertains that modifications may be made without departure from the spirit and scope of the invention. For example, although the means by which the cantilever is supported within the vessel 19 is described in accordance with the above exemplary embodiment as a slot, molded in place, internal mounting provisions to secure the cantilever, the spring and the piezoelectric stack using suitable fasteners or a suitably chosen adhesive may be employed without departing from the invention. Alternatively, subsequently drilled holes that accommodate fasteners extending through the walls or top of the vessel 19 to retain the internal component or components in place can be employed, again without departure from the invention. These holes would, of course, be sealed by a suitable sealant, as previously described.
Also, while in the above-described exemplary embodiment, the cantilever 19, the piezoelectric activator 16 and the spring 18 are distinct components, Sulchek et al. in the writing cited above, describe an integrated cantilever and piezoelectric element that could be used without departure from the present invention.
Further modifications, alterations and additions to the invention embodiments disclosed may be made without departure from the spirit and scope of the invention as set forth in the appended claims.
This application claims priority from U.S. provisional patent application Ser. No. 60/551,731 of the same title, filed Mar. 9, 2004 in the name of Yuri Lyubchenko. That application is hereby incorporated herein by reference.
Number | Date | Country | |
---|---|---|---|
60551731 | Mar 2004 | US |