TY - JOUR
T1 - Coverage dependence of LEED arced streak intensities for Li adsorption on Cu(001) surface
AU - Mitani, Hisashi
AU - Mizuno, Seigi
AU - Tochihara, Hiroshi
AU - Hayashi, Tohru
PY - 2005/10
Y1 - 2005/10
N2 - The coverage dependence of arced streak intensities observed in LEED pattern, for Li on Cu(001) surface at low coverage, (0 - 0.50), is studied theoretically. The streaks essentially originate from the deviation of numbers of adatoms on sublattice sites. In a lattice gas adsorption model, we can see two sublattices in terms of a phase on a wave number ky = 2π=2a, which corresponds to the streaks. Then we calculate an expectation value for the deviation of numbers of adatoms on the two sublattice sites, for a given coverage. This deviation brings an atomic density wave and also gives an intensity of the streak. The calculated coverage dependence of the intensity is similar to the experiment. In the real experimental system, the streaks are expanded and deformed in diffraction space. It means inclined or incommensurate atomic density wave. Even in such a case, we show that the above two sublattice model is essentially sufficient.
AB - The coverage dependence of arced streak intensities observed in LEED pattern, for Li on Cu(001) surface at low coverage, (0 - 0.50), is studied theoretically. The streaks essentially originate from the deviation of numbers of adatoms on sublattice sites. In a lattice gas adsorption model, we can see two sublattices in terms of a phase on a wave number ky = 2π=2a, which corresponds to the streaks. Then we calculate an expectation value for the deviation of numbers of adatoms on the two sublattice sites, for a given coverage. This deviation brings an atomic density wave and also gives an intensity of the streak. The calculated coverage dependence of the intensity is similar to the experiment. In the real experimental system, the streaks are expanded and deformed in diffraction space. It means inclined or incommensurate atomic density wave. Even in such a case, we show that the above two sublattice model is essentially sufficient.
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U2 - 10.1143/JPSJ.74.2663
DO - 10.1143/JPSJ.74.2663
M3 - Article
AN - SCOPUS:27144498268
SN - 0031-9015
VL - 74
SP - 2663
EP - 2666
JO - journal of the physical society of japan
JF - journal of the physical society of japan
IS - 10
ER -