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(a)
10
5
0
-5
-10
0
2
4
6
8
10
Energy (eV)
(b)
10
8
6
4
2
0
- /( a + b )
0
/( a + b )
Figure 3.4 (a) The horizontal dashed lines at + 1 and at 1 show the upper and lower
limits of the left-hand side of eq. (3.13). The smooth curve shows how the
right-hand side of eq. (3.13), f R ( E ) , varies with energy E for the case where
a = 5Å, b = 1.5 Å and V 0 = 10 eV. It can be seen that there are only
certain bands of energy where there can be allowed solutions of eq. (3.13)
(around 1, 4, and 8 eV in this case), separated from each other by energy
gaps where there are no allowed solutions. (b) shows the band structure
in the K-P model, with energy plotted against wavenumber q for the case
considered in (a) ( a = 5Å, b = 1.5 Å and V 0 = 10 eV). It can be seen that
the band edges occur at q = 0or π/ ( a + b ), that is, where the left-hand
side of eq. (3.13) equals ± 1.
with energy, E , of the right-hand side of eq. (3.14), f R
, superimposed
on a graph of the range of allowed values of the left-hand side, showing
clearly the existence of allowed and forbidden energy regions.
Figure 3.4(b) shows the calculatedband structure for theK-Pmodel, with
E plotted against q in the first Brillouin zone (for which
(
E
)
|
|≤ π/(
+
))
q
a
b
,
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