C60 / Corannulene on Cu(110)
(Result of the month 12/2008)

A Surface-Supported Bistable Buckybowl-Buckyball Host-Guest System


Corannulene (COR) buckybowls were proposed as near ideal hosts for fullerene C60, but direct complexation of C60 and COR has remained a challenge in supramolecular chemistry. We report the formation of surface-supported COR-C60 host-guest complexes by deposition of C60 onto a COR lattice on Cu(110). Variable-temperature scanning tunneling microscopy studies reveal two distinctly different states of C60 on the COR host lattice, with different binding energies and bowl-ball separations. The transition from a weakly bound precursor state to a strongly bound host-guest complex is found to be thermally activated. Simple model calculations show that this bistability originates from a subtle interplay between homo- and heteromolecular interactions.

The COR host lattice:
(a) STM image of a COR monolayer on Cu(110) revealing enantiomorphous a  and r  domains. High-symmetry directions of the Cu(110) surface (black arrows) and the close-packed directions of the COR lattice (white arrows) are indicated.
(b) Highresolution STM image revealing the bowl shape of COR.
(c) Structural model of the F-domain with molecular orientations as determined from XPD experiments.A 6° tilt of the C5σ axis along the [110] direction causes a C-C bond between a C6 and the C5 ring (highlighted in yellow) being closest to the surface.
(d) Schematic illustration of the surface-supported COR host lattice, with some of the host sites occupied by fullerene C60 guests.



Manipulating C60 molecules away from their original positions by an abrupt reduction of the gap voltage from -1.2 V to -0.02 V during scanning.
a) STM image with normal tunnelling parameters after deposition of ~1 ML C60 onto the COR host lattice at ET. The white arrow indicates the position where an abrupt reduction of the gap voltage is applied during the scanning.
b) After an abrupt reduction of the gap voltage, some C60 molecules were swept away and small C60 vacancy islands ("B”) were created. This tip created C60 vacancy islands ("B”) has an identical apparent depth as the original one ("A”) with respect to the C60 aggregates, suggesting that the C60 molecules are directly located on top of underlying COR bowls.


Data Courtesy of:
Wende Xiao(1), Daniele Passerone(1), Pascal Ruffieux (1), Kamel Aït-Mansour(1), Oliver Gröning (1), Erio TosattiC Jay S. Siegel(3) and Roman Fasel(1)

(1)
nanotech@surfaces Laboratory, Empa, Swiss Federal Laboratories for Materials Testing and Research,  3602 Thun, Switzerland and 8600 Dübendorf, Switzerland
(2) International School for Advanced Studies, INFM/CNR/DEMOCRITOS, and International Centre for Theoretical Physics, 34014 Trieste, Italy
(3) Department of Organic Chemistry, UniVersity of Zurich, Zurich, Switzerland

Corresponding Author:
roman.fasel@empa.ch

Publications:
J. AM. Chem. Soc. 2008, 130, 4767-4771

 
This result has been obtained with :
Variable Temperature UHV SPM

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