1. (a) Show that along the principal symmetry directions shown in Figure 10.5 the tight- binding expression (10.22) for the energies of an s-band in a face-centered cubic crystał reduces to the following: (i) Ałong rX (k, = k̟ = 0, kg = µ 2m/a, 0 < µ < 1) 8 = E, – B – 4y(1 + 2 cos µn). %3D %3D (ii) Along TL (k, = k, = k, = µ 2n/a, 0 < H< }) %3D %3D 8 = E, – B - 12y cos²µn. (iii) Along TK (k, = 0, kg = k, = µ 27/a, 0 < µ < ) %3D %3D 8 = E, -- B - 4y(cos² µn + 2 cos µn). (iv) Along rW (k̟ = 0, k, = µ 2n/a, ky fu 2n/a, 0 < µ < 1) %3D E-β- 4γ(cos μπ + cos μπ + os μπ cos μπ ).
1. (a) Show that along the principal symmetry directions shown in Figure 10.5 the tight- binding expression (10.22) for the energies of an s-band in a face-centered cubic crystał reduces to the following: (i) Ałong rX (k, = k̟ = 0, kg = µ 2m/a, 0 < µ < 1) 8 = E, – B – 4y(1 + 2 cos µn). %3D %3D (ii) Along TL (k, = k, = k, = µ 2n/a, 0 < H< }) %3D %3D 8 = E, – B - 12y cos²µn. (iii) Along TK (k, = 0, kg = k, = µ 27/a, 0 < µ < ) %3D %3D 8 = E, -- B - 4y(cos² µn + 2 cos µn). (iv) Along rW (k̟ = 0, k, = µ 2n/a, ky fu 2n/a, 0 < µ < 1) %3D E-β- 4γ(cos μπ + cos μπ + os μπ cos μπ ).
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Transcribed Image Text:L
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![1. (a) Show that along the principal symmetry directions shown in Figure 10.5 the tight-
binding expression (10.22) for the energies of an s-band in a face-centered cubic crystał reduces
to the following:
(i) Ałong TX (k, = k̟ = 0, kg =µ 27/a,
0 < µ< 1)
%3D
8 = E, - B – 4y(1 + 2 cos µn).
(ii) Along FL (k, = k, = k, = µ 2n/a,
0 < µ< )
8 = E, – B -- 12y cos²µn.
( i) Along ΓΚ (,0, k-k,= μ 2π/α,
0 < µ < )
%3D
8 =
-E-β- 4γ(cos μπ +2cos μπ).
(iv) Along rW (k,
0, k, = µ 27/a, k, = }µ 2n/a,
0 <µ < 1)
8 = E, – B – 4y(cos µn + cos ¿un + cos µn cos žuT).
%3D
(b) Show that on the square faces of the zone the normał derivative of ɛ vanishes.
(c) Show that on the hexagonał faces of the zone, the normał derivative of Ɛ vanishes onły
ałong lines joining the center of the hexagon to its vertices.](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F800cdc5c-856b-42f7-bca2-db86bfaf45e0%2Fd0033245-ca11-449c-8b13-0ad937497c20%2Flix09m_processed.png&w=3840&q=75)
Transcribed Image Text:1. (a) Show that along the principal symmetry directions shown in Figure 10.5 the tight-
binding expression (10.22) for the energies of an s-band in a face-centered cubic crystał reduces
to the following:
(i) Ałong TX (k, = k̟ = 0, kg =µ 27/a,
0 < µ< 1)
%3D
8 = E, - B – 4y(1 + 2 cos µn).
(ii) Along FL (k, = k, = k, = µ 2n/a,
0 < µ< )
8 = E, – B -- 12y cos²µn.
( i) Along ΓΚ (,0, k-k,= μ 2π/α,
0 < µ < )
%3D
8 =
-E-β- 4γ(cos μπ +2cos μπ).
(iv) Along rW (k,
0, k, = µ 27/a, k, = }µ 2n/a,
0 <µ < 1)
8 = E, – B – 4y(cos µn + cos ¿un + cos µn cos žuT).
%3D
(b) Show that on the square faces of the zone the normał derivative of ɛ vanishes.
(c) Show that on the hexagonał faces of the zone, the normał derivative of Ɛ vanishes onły
ałong lines joining the center of the hexagon to its vertices.
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