Resonant core spectroscopies of the charge transfer interactions between C60 and the surfaces of Au(111), Ag(111), Cu(111) and Pt(111)

Research paper by Andrew J. Gibson, Robert H. Temperton, Karsten Handrup, James N. O'Shea

Indexed on: 27 Nov '16Published on: 27 Nov '16Published in: Surface Science (including Surface Science Letters)


Charge transfer interactions between C60 and the metal surfaces of Ag(111), Cu(111), Au(111) and Pt(111) have been studied using synchrotron-based photoemission, resonant photoemission and X-ray absorption spectroscopies. By placing the X-ray absorption and valence band spectra on a common binding energy scale, the energetic overlap of the unoccupied molecular orbitals with the density of states of the underlying metal surface have been assessed in the context of possible charge transfer pathways. Resonant photoemission and resonant Auger data, measuring the valence region as a function of photon energy for C60 adsorbed on Au(111) reveals three constant high kinetic energy features associated with Auger-like core-hole decay involving an electron transferred from the surface to the LUMO of the molecule and electrons from the three highest occupied molecular orbitals, respectively and in the presence of ultra-fast charge transfer of the originally photoexcited molecule to the surface. Data for the C60/Ag(111) surface reveals an additional Auger-like feature arising from a core-hole decay process involving more than one electron transferred from the surface into the LUMO. An analysis of the relative abundance of these core-hole decay channels estimates that on average 2.4 ±0.3 electrons are transferred from the Ag(111) surface into the LUMO. A core-hole clock analysis has also been applied to assess the charge transfer coupling in the other direction, from the molecule to the Au(111) and Ag(111) surfaces. Resonant photoemission and resonant Auger data for C60 molecules adsorbed on the Pt(111) and Cu(111) surfaces are shown to exhibit no super-Auger features, which is attributed to the strong modification of the unoccupied molecular orbitals arising from stronger chemical coupling of the molecule to the surface.

Graphical abstract 10.1016/j.susc.2016.11.009.jpg
Figure 10.1016/j.susc.2016.11.009.0.jpg
Figure 10.1016/j.susc.2016.11.009.1.jpg
Figure 10.1016/j.susc.2016.11.009.2.jpg
Figure 10.1016/j.susc.2016.11.009.3.jpg
Figure 10.1016/j.susc.2016.11.009.4.jpg
Figure 10.1016/j.susc.2016.11.009.5.jpg
Figure 10.1016/j.susc.2016.11.009.6.jpg
Figure 10.1016/j.susc.2016.11.009.7.jpg