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Rocking-motion-induced charging of C60 on hBNNi(111)

M. Muntwiler, W. Auwärter, A. P. Seitsonen, J. Osterwalder, and T. Greber
Phys. Rev. B 71, 121402(R) – Published 11 March 2005

Abstract

One monolayer of C60 on one monolayer of hexagonal boron nitride on nickel is investigated by photoemission. Between 150 and 250K the work function decreases and the binding energy of the highest-occupied molecular orbital increases by 100meV. In parallel, the occupancy of the—in the cold state almost empty—lowest unoccupied molecular orbital (LUMO) changes by 0.4±0.1 electrons. This charge redistribution is triggered by the onset of molecular rocking motion, i.e., by orientation dependent tunneling between the LUMO of C60 and the substrate. The magnitude of the charge transfer is large and cannot be explained within a single-particle picture. It is proposed to involve electron-phonon coupling where C60 polaron formation leads to electron self-trapping.

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  • Received 19 November 2004

DOI:https://doi.org/10.1103/PhysRevB.71.121402

©2005 American Physical Society

Authors & Affiliations

M. Muntwiler1, W. Auwärter1, A. P. Seitsonen2, J. Osterwalder1, and T. Greber1

  • 1Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
  • 2Physikalisch-Chemisches Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland

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Vol. 71, Iss. 12 — 15 March 2005

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Images

  • Figure 1
    Figure 1
    The investigated system C60hBNNi(111). (a) Sketch of the interface. (b) STM picture of the well-ordered monolayer of C60. The three gray levels indicate three different terraces on the substrate. (c), (d) LEED patterns (E=23.5eV): (4×4) at 250K and (43×43)R30° at 160K.Reuse & Permissions
  • Figure 2
    Figure 2
    He Iα photoemission spectra of one monolayer of C60 on hBNNi(111) for room temperature and 140K. The inset shows the strong shift of the photoemission leading edge that is due to the population of the LUMO at high temperatures.Reuse & Permissions
  • Figure 3
    Figure 3
    Occupancy of the LUMO (solid circles) and the normal emission HOMO intensity (open triangles) as a function of reciprocal temperature. The solid lines are guides to the eye. The inset shows the extrapolated LUMO from the 300K data in Fig. 2.Reuse & Permissions
  • Figure 4
    Figure 4
    Deviation of the LUMO of C60 from spherical symmetry. (a) Constant electron density isosurface. (b) Stereographic projection of the integral electron density outside planes placed 5Å away from the center of C60. The low density parallel to hexagons (center of the plot) and the high density parallel to pentagons is apparent. The bottom panel shows the anisotropy of this electron density that is related to the tunneling rate between the substrate and the molecule along the dashed θ line. The tunneling anisotropy of 1 corresponds to the average of all molecular orientations.Reuse & Permissions
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