Au 20 : A Tetrahedral Cluster

American Association for the Advancement of Science (AAAS) - Tập 299 Số 5608 - Trang 864-867 - 2003
Jun Li1, Xi Li2,1, Hua‐Jin Zhai2,1, Lai-Sheng Wang2,1
1W. R. Wiley Environmental Molecular Sciences Laboratory, Pacific Northwest National Laboratory, Post Office Box 999, Richland, WA 99352, USA.
2Department of Physics, Washington State University, 2710 University Drive, Richland, WA 99352, USA

Tóm tắt

Photoelectron spectroscopy revealed that a 20-atom gold cluster has an extremely large energy gap, which is even greater than that of C 60 , and an electron affinity comparable with that of C 60 . This observation suggests that the Au 20 cluster should be highly stable and chemically inert. Using relativistic density functional calculations, we found that Au 20 possesses a tetrahedral structure, which is a fragment of the face-centered cubic lattice of bulk gold with a small structural relaxation. Au 20 is thus a unique molecule with atomic packing similar to that of bulk gold but with very different properties.

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Tài liệu tham khảo

10.1038/318162a0

10.1038/347354a0

M. A. Hayat Ed. Colloidal Gold: Principles Methods and Applications (Academic Press New York 1989).

10.1126/science.281.5383.1647

Heiz U., Schneider W. D., J. Phys. D Appl. Phys. 33, R85 (2000).

10.1021/jp9935992

Lopez N., Nørskov J. K., J. Am. Chem. Soc. 124, 11262 (2002).

10.1126/science.1076248

10.1126/science.277.5329.1078

10.1126/science.280.5372.2098

Whetten R. L., et al., Acc. Chem. Res. 32, 397 (1999).

10.1021/ar9602664

Luedtke W. D., Landman U., J. Phys. Chem. 100, 13323 (1996).

Häberlen O. D., Chung S. C., Stener M., Rösch N., J. Chem. Phys. 106, 5189 (1997).

Garzón I. L., et al., Phys. Rev. Lett. 81, 1600 (1998).

Bonacic-Koutecky V., et al., J. Chem. Phys. 117, 3120 (2002).

Gilb S., Weis P., Furche F., Ahlrichs R., Kappes M. M., J. Chem. Phys. 116, 4094 (2002).

Häkkinen H., Moseler M., Landman U., Phys. Rev. Lett. 89, 033401 (2002).

Furche F., et al., J. Chem. Phys. 117, 6982 (2002).

10.1063/1.1149694

L. S. Wang X. Li in Cluster and Nanostructure Interfaces P. Jena S. N. Khanna B. K. Rao Eds. (World Scientific Singapore 2000) pp. 293–300

Tarlor K. J., Pettiette-Hall C. L., Cheshnovsky O., Smalley R. E., J. Chem. Phys. 96, 3319 (1992).

Wang L. S., Cheng H. S., Fan J., J. Chem. Phys. 102, 9480 (1995).

Wang X. B., Ding C. F., Wang L. S., J. Chem. Phys. 110, 8217 (1999).

Gunnarsson O., et al., Phys. Rev. Lett. 74, 1875 (1995).

de Heer W. A., Rev. Mod. Phys. 65, 611 (1993).

Pyykkö P., Runeberg N., Angew. Chem. Int. Ed. 41, 2174 (2002).

Li X., Kiran B., Li J., Zhai H. J., Wang L. S., Angew. Chem. Int. Ed. 41, 4786 (2002).

Relativistic density functional calculations on Au 20 and its anion were performed at the level of a generalized gradient approach using a Perdew-Wang exchange-correlation functional (30). The zero-order regular approximation Hamiltonian was used to account for the scalar (mass velocity and Darwin) and spin-orbit relativistic effects (31). The standard Slater-type orbital basis sets with quality of triple-zeta plus p - and f -polarization functions (TZ2P) were used for the valence orbitals of the Au atoms with frozen core approximation to the [1 s 2 -4 f 14 ] core. The vertical detachment energies of the anions were calculated via the self-consistent field energy difference between the neutral and anion ground states and the excitation energies of the neutral state calculated by the time-dependent density functional theory method (32). All the calculations were accomplished with the Amsterdam Density Functional (ADF 2002) program (33). We found that these theoretical methods are suitable for smaller gold clusters as well as for gold clusters doped with an impurity atom (28).

Perdew J. P., Wang Y., Phys. Rev. B 45, 13244 (1992).

van Lenthe E., Baerends E. J., Snijders J. G., J. Chem. Phys. 99, 4597 (1993).

van Gisbergen S. J. A., Snijders J. G., Baerends E. J., Comput. Phys. Commun. 118, 119 (1999).

ADF 2002 SCM Theoretical Chemistry Vrije Universiteit Amsterdam Netherlands (www.scm.com).

Prinzbach H., et al., Nature 407, 60 (2000).

N. T. Wilson R. L. Johnston Eur. Phys. J. D 12 161 (2000).

J. Wang G. Wang J. Zhao Phys. Rev. B 66 354181 (2002).

Nilius N., Wallis T. M., Ho W., Science 297, 1853 (2002).

The calculations show that the A B and C peaks in the PES spectra (Fig. 1) correspond to the triplet and singlet states formed by electron detachment from the HOMO (16e) and HOMO-1 (29t 2 ) wheras the D and E peaks are due to transitions from HOMO-2 (18t 1 ). See the supporting online material (fig. S1) for the molecular orbital energy-level diagram of T d Au 20 .

Preliminary calculations on four CO molecules absorbed on the apex and face-center sites reveal a HOMO-LUMO gap of 1.43 and 1.50 eV for the Au 20 (CO) 4 clusters and a binding energy of 0.84 and 0.15 eV per CO molecule respectively. The large HOMO-LUMO gaps in the naked and CO-adsorbed clusters indicate that the T d Au 20 is highly chemically inert and will maintain its structural integrity during catalysis.

We thank B. Kiran for helpful discussion. This work was supported by NSF (grant CHE-9817811) and performed at the Environmental Molecular Sciences Laboratory (EMSL) a national scientific user facility sponsored by the U.S. Department of Energy's (DOE's) Office of Biological and Environmental Research and located at Pacific Northwest National Laboratory operated for DOE by Battelle. All the calculations were performed with supercomputers at the EMSL Molecular Science Computing Facility.