In tapping mode atomic force microscopy, the cantilever tip intermittently taps the sample as the tip scans over the surface. This mode is suitable for imaging fragile samples such as biological macromolecules, because vertical oscillation of the cantilever reduces lateral forces between the tip and sample. However, the tapping force (vertical force) is not necessarily weak enough for delicate samples, particularly for biomolecular systems containing weak inter- or intramolecular interactions. Light tapping requires an amplitude set point (i.e., a constant cantilever amplitude to be maintained during scanning) to be set very close to its free oscillation amplitude. However, this requirement does not reconcile with fast scans, because, with such a set point, the tip may easily be removed from the surface completely. This article presents two devices to overcome this difficulty; a new feedback controller (named as “dynamic proportional-integral-differential controller”) and a compensator for drift in the cantilever-excitation efficiency. Together with other devices optimized for fast scan, these devices enable high-speed imaging of fragile samples.
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August 2006
Research Article|
August 31 2006
Dynamic proportional-integral-differential controller for high-speed atomic force microscopy
Noriyuki Kodera;
Noriyuki Kodera
Department of Physics,
Kanazawa University
, Kakuma-machi, Kanazawa 920-1192, Japan
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Mitsuru Sakashita;
Mitsuru Sakashita
Department of Physics,
Kanazawa University
, Kakuma-machi, Kanazawa 920-1192, Japan
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Toshio Ando
Toshio Ando
Department of Physics,
Kanazawa University
, Kakuma-machi, Kanazawa 920-1192, Japan and CREST
, JST, 4-1-8 Honcho Kawaguchi, Saitama 332-0012, Japan
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Rev. Sci. Instrum. 77, 083704 (2006)
Article history
Received:
April 04 2006
Accepted:
July 10 2006
Citation
Noriyuki Kodera, Mitsuru Sakashita, Toshio Ando; Dynamic proportional-integral-differential controller for high-speed atomic force microscopy. Rev. Sci. Instrum. 1 August 2006; 77 (8): 083704. https://doi.org/10.1063/1.2336113
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