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Imaging of molecular orbitals and bond formation

Project overview

Insulating films with a thickness of only a few atomic layers residing on a conducting substrate provide sufficient electronic decoupling to allow us to study the inherent electronic properties of individual molecules. As electrons can tunnel through these ultrathin films, adsorbates can stilll be imaged with a scanning tunneling microscope. In the example shown here of individual pentacene molecules on one, two, and three layers of NaCl on copper surfaces, we used this technique to image molecular orbitals directly. STM images (see Fig. 1) acquired at bias voltages corresponding to the negative (NIR) and positive ion resonance (PIR) perfectly resemble the structures of the lowest unoccupied (LUMO) and highest occupied (HOMO) molecular orbital of the free molecule, that is, the bare molecule in vacuum. This opens up the fascinating and unprecedented possibility to obtain direct images of native molecular orbitals, completely disentangled from the electronic structure of the substrate.

Molecular orbitals depend critically on the detailed molecular structure. Single-molecule chemistry by scanning probe manipulation allows the controlled breaking and formation of individual bonds. Molecular orbital imaging in conjunction with single-molecule chemistry introduces a new way to follow bond formation with utmost detail. We have studied the bond formation between a single gold atom and a pentacene molecule employing molecular imaging. Of particular interest is the buildup of metal molecule complexes, which are also the first step towards controlled electronic contacting of single molecules. Figure 2 shows the bond formation between a pentacene molecule and a gold atom on a bilayer of NaCl. In Fig. 2A, the reactants are already located close to each other. The bond was formed by inelasting tunneling (IET), and the resulting complex (Fig. 2B) has a mirror plane that is perpendicular to the long axis of the molecule, indicating that the gold atom is attached to the central ring of pentacene (6-gold-pentacene) (Figs. 2C and D). The bond can be broken again by IET-induced excitation of the entire complex. Different Au-pentacene isomers were formed with this technique. The reversibility of the complex formation suggests that it is an additional reaction of the gold atom to one of the pentacene's aromatic rings and involves neither the substitution of a hydrogen atom nor the creation of a defect in the substrate.

The gold-pentacene complexes exhibit two peaks in their dI/dV spectrum, as in case of the individual pentacene molecule, but with a much smaller gap. Orbital images taken at occupied and unoccupied states are very similar, indicating that tunneling in and out involves the same orbital (Fig. 3). Indeed, detailed STM experiments indicate that Au-pentacence is neutral, therefore electron counting shows directly that Au-pentacene has one orbital that is only singly occupied. (SOMO: singly occupied molecular orbital).

These experiments have been supported by theoretical calculations performed by the groups of C. Joachim (CEMES Toulouse) and M. Persson (University of Liverpool).

 References

J. Repp, G. Meyer, S. Stojkovic, A. Gourdon, C. Joachim, Physical Review Letters 94, 026803 (2005).

J. Repp, G. Meyer, S. Paavilainen, F. Olsson, M. Persson, Science 312, 1197 (2006).

Images, click to enlarge
Figure 1. STM images of a pentacene molecule on a two-atomic-layer-thick NaCl film on Cu(111).
Pentacene molecule
Figure 2. Making and breaking a chemical bond between a single pentacene molecule and Au atom on an NaCl bilayer on Cu(100).
chemical bond
Figure 3. Orbital images of the 6-gold pentacene complex.
6-gold pentacene complex
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