A tenser LEED analysis of the Pd(100)-(root 5 x root 5)R27 degrees-O s
urface structure supports a surface oxide model, as first postulated b
y Orent and Bader. The detailed model which gives the best corresponde
nce with experimental intensity data has a PdO(001) overlayer stacked
on to the Pd(100) surface such that rumpling is induced in both the ox
ide and topmost Pd(100) layers. The structure can be seen as represent
ing a compromise between the drive toward an ideally flat PdO(001) sur
face and the need to optimize total bonding at the surface. Pd atoms i
n the topmost Pd(100) layer appear to displace laterally to minimize c
orrugations in the top metal layers. The total corrugations in the PdO
overlayer and the first Pd(100) layer are indicated to be about 0.26
and 0.51 Angstrom, respectively. The average O-Pd bond length for two-
coordinate O on the Pd surface (1.73 Angstrom) remains dose to the pre
dicted value of 1.76 Angstrom based on the structure of bulk PdO.