Abstract. Nanosecond laser pulses are used to illuminate the very end of a tip of a scanning tunneling microscope in front of a gold surface. The transient increase of the tunneling current is measured as a function of the pulse energy density, tip retraction amplitude, polarization of the incident light, and bias voltage. The transient signal has a typical timescale of ms. Thus it can be concluded that the thermal expansion of the tip is responsible for this signal. The expansion has a linear dependence on the incident light intensity with a typical value of the order of 0.1 Å/(mJ/cm 2 ). This result demands a critical inspection of the interpretation of nanostructuring experiments with this technique.
PACS: 6116P; 6570; 4260KThe scanning tunneling microscope and the atomic force microscope are frequently used for the production of nanostructures on surfaces. Whereas the possible use of forces or electric fields is already known from different applications [1] another quite new idea is the external injection of laser radiation into the tip-substrate gap. It has been shown that by using this technique nanostructures of different forms can be produced [2][3][4][5][6]. Even reliable single-atom deposition is achievable [5]. The physical reasons for these possibilities are not clear. On one hand it is proposed that the metallic tip produces a local enhancement of the optical radiation similar to the well-known surface-enhanced Raman effect [2][3][4]6]. On the other hand the possibility of thermal expansion and therefore of mechanical contact is also discussed [5].In order to clarify this situation we have performed STM experiments in combination with the use of nanosecond laser pulses. Although a direct access to nanosecond time-resolved measurements is not possible with our present setup, we used different schemes of indirect measurements to learn about the interaction of the nanosecond laser pulse with the tip of a scanning tunneling microscope. From these experiments we conclude that thermal expansion of the tip cannot be neglected in experiments with nanosecond laser pulses but may even be the dominating mechanism involved.