Three recent articles [T.D. Pope, M. Vos, H.T. Tang, K. Griffiths, I.V
. Mitchell, P.R. Norton, W. Liu, Y.S. Li, I. Stensgaard, E. Laegsgaard
, F. Besenbacher, Surf. Sci. 337 (1995) 79; J. Yao, Y.G. Shen, D.J. O'
Connor, B.V. King, Surf. Sci. 359 (1996) 65; P.W. Murray, I. Stensgaar
d, E. Laegsgaard, F. Besenbacher, Surf. Sci. 365 (1996) 591] have atte
mpted to determine the surface composition and structure of the (2 x 2
)p4g phase induced by one monolayer (ML) Pd deposition at room tempera
ture on a Cu(001) surface. In order to remove inconsistencies arising
from previous studies, the 1 ML Pd/Cu(001) surface has been reinvestig
ated using low-energy ion scattering (LEIS), low-energy electron diffr
action (LEED), three-dimensional (3D) classical scattering simulations
and embedded-atom method (EAM) calculations. Using Li+ and He+ ion sc
attering with calibration measurements on reference samples of Cu(001)
and Pd(001), the surface Pd composition of the 1 ML phase was indepen
dently determined to be 53+/-4% and 51+/-3%, respectively. The results
obtained using K+ ion scattering, LEED and computer simulations are c
onsistent with a surface structure which consists of 30% of a clock-ro
tated (001) Pd phase and 70% of an unreconstructed p(2 x 2) Cu-Pd phas
e. The stability of the (2 x 2)p4g phase has been confirmed by EAM cal
culations. (C) 1997 Elsevier Science B.V.