Abstract
Scanning tunneling microscopy (STM) was invented by Binnig and Rohrer (see Fig. 2.1) [2,9]. Using the combination of a coarse approach and piezoelectric transducers, a sharp, metallic probing tip is brought into close proximity with the sample. The distance between tip and sample is only a few angstrom units, which means that the electron wave functions of tip and sample start to overlap. A bias voltage between tip and sample causes electrons to tunnel through the barrier. The tunneling current is in the range of pA to nA and is measured with a preamplifier.1 This signal is the input signal of the feedback loop, which is designed to keep the tunneling current constant during (x, y)-scanning. The output signal is amplified (high voltage amplifier) and connected to the z-piezo. According to the feedback output voltage and the sensitivity of the piezo (typically nm/V) the tunneling tip is moved backwards or forwards and the tunneling current is kept constant during acquisition of the image. This operation mode is called constant current mode.
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© 2004 Springer-Verlag Berlin Heidelberg
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Meyer, E., Hug, H.J., Bennewitz, R. (2004). Introduction to Scanning Tunneling Microscopy. In: Scanning Probe Microscopy. Advanced Texts in Physics. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-662-09801-1_2
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DOI: https://doi.org/10.1007/978-3-662-09801-1_2
Publisher Name: Springer, Berlin, Heidelberg
Print ISBN: 978-3-642-07737-1
Online ISBN: 978-3-662-09801-1
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