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excess coverage. On the other hand, the spot positions due to the (223) facet struc-
ture remain fixed, i.e., the additional coverage and the associated additional elec-
tron density do not change the terrace structure of the (223) surface orientation. An
example is shown in the top part of Fig. 9.7 . Here the splitting is 5.3% SBZ for 1.35
1.35ML
10 6
Δ
k (223) =21.3%SBZ
10 5
Δ
k deco =
5.3%SBZ
10 4
-25 -20 -15 -10 -5 0 5 10 15
k || [1 1 2] (%SBZ)
Fig. 9.7 Top : Exemplary line scan in LEED taken along the [112
direction for a Pb coverage
of 1.35 ML together with fits of new satellite peaks (see text). Pb layers were adsorbed at 75 K
substrate temperature. Bottom : Plot of reciprocal lattice vectors of the satellite peaks versus the Pb
excess coverage
]
(relative to 1.31 ML). The solid ( blue ) curves represent the Fermi wave vector
k F , 1D of a 1D electron gas induced by the Pb excess coverage assuming a valence state of 2. The
coincidence of 2 k F ( dashed-dotted (red) line ) with the lattice vectors of the superlattice results in
nesting
δ
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