TY - JOUR
T1 - Tensor LEED analysis of the Ni(111) (root3xroot3)R30o-Pb Surface
AU - Quinn, P. D.
AU - Bittencourt Papaleo Montes, Carla
AU - Woodruff, D. P.
PY - 2002
Y1 - 2002
N2 - The structure of the Ni(111)(√3×√3)R30°−Pb surface has been determined by quantitative low-energy electron diffraction (LEED), using multiple-scattering simulations of the measured diffracted beam intensities with a tensor-LEED program. The results confirm that the surface comprises a single-layer substitutional alloy of stoichiometry Ni2Pb (with all atoms in “fcc” sites relative to the underlying Ni) and clearly excludes a surface/subsurface stacking fault (with occupation of “hcp” sites) like that found for similar phases of Sb on Cu(111) and Ag(111). Within the surface alloy layer the Pb atoms are 0.73±0.05−Å higher above the surface than the surrounding Ni atoms in the alloy layer. This magnitude of rumpling is in excellent agreement with a recent medium-energy ion scattering investigation of this surface, but is significantly larger than that of an earlier low-energy ion scattering investigation. Compared to the rumpling amplitude of 1.67 Å expected from a simple hard-sphere model based on bulk metallic radii, however, it confirms a strong reduction of the effective atomic radii in this surface alloy.
AB - The structure of the Ni(111)(√3×√3)R30°−Pb surface has been determined by quantitative low-energy electron diffraction (LEED), using multiple-scattering simulations of the measured diffracted beam intensities with a tensor-LEED program. The results confirm that the surface comprises a single-layer substitutional alloy of stoichiometry Ni2Pb (with all atoms in “fcc” sites relative to the underlying Ni) and clearly excludes a surface/subsurface stacking fault (with occupation of “hcp” sites) like that found for similar phases of Sb on Cu(111) and Ag(111). Within the surface alloy layer the Pb atoms are 0.73±0.05−Å higher above the surface than the surrounding Ni atoms in the alloy layer. This magnitude of rumpling is in excellent agreement with a recent medium-energy ion scattering investigation of this surface, but is significantly larger than that of an earlier low-energy ion scattering investigation. Compared to the rumpling amplitude of 1.67 Å expected from a simple hard-sphere model based on bulk metallic radii, however, it confirms a strong reduction of the effective atomic radii in this surface alloy.
U2 - 10.1103/PhysRevB.65.233404
DO - 10.1103/PhysRevB.65.233404
M3 - Article
SN - 1098-0121
VL - 65
JO - Physical Review. B, Condensed Matter and Materials Physics
JF - Physical Review. B, Condensed Matter and Materials Physics
IS - 23
ER -