By the method of in situ Hall effect measurements at room temperature, it w
as shown that the formation of a clean Si(111)(7 x 7) surface at high tempe
rature annealing (T = 1250 degrees, t = 120-180 s) of n-type conductivity s
ilicon results in a change of the majority carriers on a surface. But on a
surface of p-type conductivity silicon it results in the formation of a hol
e accumulated layer. Various dynamics of changes in the Hall voltage and re
sistivity voltage within the limits of the first monolayer of room temperat
ure adsorption of iron and chromium on substrates with a p-n junction and w
ith a hole accumulated layer are not connected with conductivity along an a
bsorbed layer. To understand the mechanism of conductivity in a system adso
rbed layer Fe(Cr)/Si(111)(7 x 7), it is necessary to take into account two
effects: (a) destruction of the superstructure Si(111)(7 x 7); (b) formatio
n of donor-type surface states of Fe(Cr) in the band gap of silicon. Destru
ction of the localized surface states of the superstructure Si(111)(7 x 7)
plays the greatest role, when the density of donor-type surface states is v
ery small. It corresponds to adsorption of Cr on Si(111) of p-type conducti
vity. The greatest contribution of donor-type surface states to the conduct
ivity of the surface space-charge layer was observed with adsorption of Fe
on Si(111) of n-type conductivity. Conductivity through the adsorbed iron (
chromium) layer began with a thickness more than three monolayers.