Namangan Institute of Engineering and Technology
nammti.uz
10.25.2023
Pg.244
2
),
sin(
)
(
mE
k
x
k
A
x
(7)
Ikkita chegaraviy shartdan foydalanib bo’ldik, yana bitta noma’lum -
A
qoldi.
Buni topish
uchun bizda yana normallashtirish sharti bor. Ushbu masala uchun u quyidagicha yoziladi
L
dx
x
0
2
1
)
(
(8)
Integralni xisoblaylik
1
2
2
)
sin(
)
cos(
)
(
sin
)
(
2
0
2
2
0
2
2
L
A
k
kL
kL
kL
A
dx
kx
A
dx
x
L
L
Bundan
2/L
A
. Demak, yakuniy to’lqin funksiya ko’rinishi
,
,
2
,
sin
2
)
sin(
2
)
(
1,2,3...
n
nπ
L
k
mE
k
x
L
nπ
L
x
k
L
x
n
n
n
n
n
(9)
O’ra ichida zarrachani energiyasini qabul qilish mumkin bo’lgan qiymatlari diskret bo’lib, u
quyidagiga teng
,
2
2
2
2
2
2
2
2
1,2,3...
n
mL
n
m
k
E
n
n
(10)
3-rasm
Ixtiyoriy ketma ket ikkita satx orasidagi farq (10) dan
)
1
2
(
2
2
2
2
1
n
mL
E
E
E
n
n
n
Agar bunga elektron massasi
ã
10
27
ni qo’yib,
10 ñì
L
deb (bu misolni
metalldagi erkin
elektronlar deyish mumkin) xisoblasak
eV
)
1
2
(
10
16
n
E
n
satxlar o’ta quyuq, ya’ni
tutash spektr deyish mumkin. Agar o’ra kengligin
atomlar razmerida
ñì
10
L
8
deb olinsa,
eV
)
1
2
(
10
2
n
E
n
diskretlik kuchli namoyon bo’ladi.
Foydalanilgan adabiyotlar
1.
P.J. Baymatov, B.T.Abdulazizov //
On the Thermodynamics of a Two-Dimensional Electron
Gas with Non-Parabolic Dispersion // World Journal of Condensed Matter Physics, 2016, 6, 294-299,
Published November 17, 2016 SciRes Google based IF=0.80, ResearchGate IF=0.57)
http://www.scirp.org/journal/wjcmp
,
http://dx.doi.org/10.4236/wjcmp.2016.64028
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10.25.2023
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2. Гулямов Г., Давлатов А.Б., Жураев Х.Н. Статистика электронов в полупроводниковых
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Physical
Review
B,
64,
Article
ID:
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in
InAs/AlSb
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Letters,
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5,680-685, (2014),
http://www.scirp.org/journal/jmp
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5,
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(2015),
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,
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