We investigated different kind of π–conjugated molecules in a combined scanning tunnelling (STM) and atomic force microscope (AFM). Whereas both measurement channels show features with sub-molecular resolution, the information they can provide is truly complementary. For example, STM allows the direct imaging of the unperturbed molecular orbitals [1], whereas the AFM channel directly reveals the molecular geometry [2, 3]. When applied to STM-based single-molecule synthesis and on-surface chemistry, the combination of these techniques enables a direct quantification of the interplay of geometry and electronic coupling in real space [3, 4]. In particular, in many cases only the AFM channel enables discriminating different binding sites inside a single molecule, which is a prerequisite to obtain a full atomistic description of regioselectivity in on-surface chemistry [4]. Similarly, in the case of hydrogen-bonded molecular assembly the AFM provides direct insight into the bond rearrangement upon crystallization in two dimensions [5], which is elusive for STM.
The possibility of tailoring optical waveforms has allowed scientists to steer ultrafast electronic motion directly via the oscillating carrier wave of light – a principle dubbed “lightwave electronics” [6]. Terahertz (THz) scanning tunnelling microscopy 7 has introduced a new paradigm by combining STM with lightwave electronics. In THz-STM, the electric field of a phase-stable single-cycle THz waveform acts as a transient bias voltage across an STM junction. In analogy to the all-electronic pump-probe scheme introduced recently in STM [8] these voltage transients may result in a net current that can be detected by time-integrating electronics.
By means of a low-noise low-temperature lightwave-STM we entered an unprecedented tunnelling regime, where the peak of a terahertz electric-field waveform opens an otherwise forbidden tunnelling channel through a single molecular orbital. In this way, the terahertz peak removes a single electron from an individual pentacene molecule’s highest occupied molecular orbital within a time window of ~100 fs – faster than an oscillation cycle of the terahertz wave. This quantum process allowed us to capture a microscopic real-space snapshot of the molecular orbital on a sub-cycle time scale. By correlating two successive state-selective tunnelling events, we directly tracked coherent THz vibrations of a single molecule in the time domain [9]
Figure 1. Schematic representation of the lightwave-STM setup in which the THz-pulse acts as a bias transient.
[1] J. Repp et al., Phys. Rev. Lett. 94, 026803 (2005).
[2] L. Gross et al., Science 325, 1110 (2009).
[3] F. Albrecht et al., JACS 137, 7424 (2015).
[4] N. Kocić et al., JACS 138, 5585 (2016).
[5] L. Patera et al., Angew. Chem. Int. Ed. 56, 10786 (2017).
[6] E. Goulielmakis et al., Science 317, 769 (2007).
[7] T. L. Cocker et al., Nature Photon. 7, 620 (2013)
[8] S. Loth et al., Science 329, 1628 (2010).
[9] T. L. Cocker et al., Nature 539, 263 (2016).
PCseminarabstr_171106