H. Bludau
Max Planck Society
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Featured researches published by H. Bludau.
Chemical Physics Letters | 1997
S. Schwegmann; Ari P. Seitsonen; H. Dietrich; H. Bludau; Herbert Over; Karl Jacobi; G. Ertl
Abstract The local adsoprtion geometries of the (2 × 2)-N and (✓3 × ✓3)R30°-N phases on the Ru(0001) surface are determined by analyzing low-energy electron diffraction intensity data. For both phases, nitrogen occupies the threefold hcp site. The nitrogen sinks deeply into the top Ru layer resulting in a N-Ru interlayer distance of 1.05 and 1.10 A in the (2 × 2) and the (✓3 × ✓3)R30° unit cell, respectively. This result is attributed to a strong N binding to the Ru surface (Ru-N bond length = 1.93 A ) in both phases as also evidenced by an initio calculations which revealed binding energies of 5.82 and 5.59 eV, respectively.
Physical Review B | 1998
S. Schwegmann; Ari P. Seitsonen; V. De Renzi; H. Dietrich; H. Bludau; M. Gierer; Herbert Over; Karl Jacobi; Matthias Scheffler; G. Ertl
Oxygen adsorption on to Ru(101\ifmmode\bar\else\textasciimacron\fi{}0) results in the formation of two ordered overlayers, i.e., a
Surface Science | 1994
Herbert Over; M. Gierer; H. Bludau; G. Ertl; S. Y. Tong
c(2\ifmmode\times\else\texttimes\fi{}4)\ensuremath{-}2\mathrm{O}
Chemical Physics Letters | 1994
H. Bludau; M. Gierer; Herbert Over; G. Ertl
and a
Surface Science | 1996
M. Gierer; H. Bludau; Herbert Over; G. Ertl
(2\ifmmode\times\else\texttimes\fi{}1)p2mg\ensuremath{-}2\mathrm{O}
Surface Science | 1995
H. Bludau; Herbert Over; Tobias Hertel; M. Gierer; G. Ertl
phase, which were analyzed by low-energy electron diffraction (LEED) and density functional theory (DFT) calculation. In addition, the vibrational properties of these overlayers were studied by high-resolution electron loss spectroscopy. In both phases, oxygen occupies the threefold coordinated hcp site along the densely packed rows on an otherwise unreconstructed surface. The O atoms are attached to two atoms in the first Ru layer Ru(1) and to one Ru atom in the second layer Ru(2), forming zigzag chains along the troughs. While in the low-coverage
Surface Science | 1992
M. Gierer; H. Bludau; Tobias Hertel; Herbert Over; Wolfgang Moritz; G. Ertl
c(2\ifmmode\times\else\texttimes\fi{}4)\ensuremath{-}\mathrm{O}
Surface Science | 1994
Tobias Hertel; Herbert Over; H. Bludau; M. Gierer; G. Ertl
phase, the bond lengths of O to Ru(1) and Ru(2) are 2.08 and 2.03 \AA{}, respectively, corresponding bond lengths in the high-coverage
Surface Science | 1995
Herbert Over; H. Bludau; R. Kose; G. Ertl
(2\ifmmode\times\else\texttimes\fi{}1)\ensuremath{-}p2mg\ensuremath{-}2\mathrm{O}
Surface Review and Letters | 1995
Herbert Over; H. Bludau; M. Gierer; G. Ertl
phase are 2.01 and 2.04 \AA{} (LEED). Although the adsorption energy decreases by 220 meV with O coverage (DFT calculations), we observe experimentally a shortening of the Ru(1)-O bond length with O coverage. The