A comparative study on negative ion formation in the scattering of a p
roton beam from both a clean and one monolayer of barium-covered Ag(11
1) surface is presented. The angular and energy dependence of the back
scattered negative hydrogen ions as a function of incoming and azimuth
al angles has been determined for a beam energy of 750 eV. The backsca
ttered negative particles emerge from the surface as well as from deep
er layers of the crystal. The angular dependence of the outgoing parti
cles shows a very rich structure, which is explained by shadowing and
blocking of the incoming and outgoing particles. In addition, the angu
lar dependence of the outgoing neutral particles is determined. The es
sential features appear the same, but distinct differences can be obse
rved. These are due to changes in the probability for negative ion for
mation as a function of outgoing angle. The energy distributions of th
r outgoing particles suggest a large penetration depth along the cryst
al channels. We have performed classical trajectory calculations that
simulate the angular distributions of the backscattered particles very
well. These calculations also show considerable penetration of partic
les into the bulk of the crystal and complicated zigzag trajectories t
hrough the bulk before leaving the crystal. The (electronic) stopping
inside the Ag solid is at least one or two orders of magnitude smaller
(<0.3 eV/Angstrom at E= 700 eV) than the values found in the literatu
re. Comparing the Ag(111) data and the data of Ag(111) covered by one
monolayer barium, we conclude that the barium atoms occupy lattice pos
itions of the crystal. The overlayer must contain vacancies to accommo
date the large size mismatch between the barium atoms and those of the
substrate.