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advanced semiconductor fundamentals test
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ENE 5330 Midterm Exam
Fall 2017
Name: Student number:
(b) What is the density of atoms per cm
5.43 angstrom at room temperature.
(c) Determine the center-to-center distance between the nearest neighbors in the Si lattice
(d) Calculate the density of Si at room temperature. The atomic weight of Si is 28.086 g/mol. The number of
atoms in a mole is called Avogadro's number, the value of which is approximately 6.022 ร 10
23 .
(e) Calculate the (100) and (110) surface density (# of atoms per area).
Solution
(a)
Si lattice is diamond structure, hence: there are three type of atoms in the unit cell
8 corner atoms ร
1
8
6 face atoms ร
1
2
Total of 8 atoms per unit cell.
(b)
Number of density in Si ร
8
๏ฟฝ5.43ร
โ 8 ๐๐๏ฟฝ
22
โ 3 .
(c)
From 1.(b), lattice constant for Si is 5.43ร .
โ
8
Center to center distance between the nearest neighbors is
โ
8
โ
8
(d)
Density of Si is
๐๐๐๐๐๐ ๐๐ ๐๐๐๐๐๐๐ ๐๐ ๐๐
๐ด๐ด๐๐ด๐ด๐๐๐ โฒ๐ ๐๐๐๐๐๐
22
โ
23
โ
โ
3
(e)
Surface density of (100) is
4 ร
1
4
( 5. 43 ร 10 โ8^ ๐๐)^2
14
โ
Surface density of (110) is
4 ร
1
4
+2ร
1
2
14
โ
width a. The potential energy U(x) is zero inside the well and infinity outside the well.
a) Show that the normalized wavefunction is
1
( ) x sin( x / a ) a
b) Compute < x > and provide an interpretation.
c) Compute < px > and provide an interpretation.
d) Compute
2 < p x >
e) Show that
2 2 2
2 1 0 0
p x
m m a
ฯ ฮต
, whereฮต 1 is the ground state energy.
Solution:
a) ฯ (^) ( x (^) ) = A sin (^) ( kx (^) ) + B cos( kx )
ฯ (^) ( 0 )= 0 โ B = 0
( ) 0
n a k a
( ) sin^
n x A x a
ฯ ฯ
( )
2
0
a x dx A a
โซ
( )
sin
n x x a a
1 (^ )
x sin x a a
b) (^) ( ) ( )
sin 2
a a (^) a x x x x dx x x dx a a
ฯ ฯ ฯ
โซ โซ
The expectation value of position is
2
a , which is the middle of the infinite potential well
are much larger than atomic dimension, derive an expression for the density of states (g (^) 2D) in energy.
Assume a valley degeneracy of gV.
a) Assume a parabolic dispersion near k = 0
2 2
2
C
k E E m
b) Assume a linear dispersion near k = 0
Show details of your work.
Solution:
a)
1 1
2 2
States between &
k dk k A spin kdk
States per unit energy per area @ (^1 )
V D
g dk E g k
2 2
C C C
k m E E dk m E E k m dE E E
โ = + โ = โ = โ
(^2 )
V V D
g dk g m g k
b)
C F F F
E E dk E E k k dE
(^2 2 )
2 for positive and negative
V V C D F
g dk g E E g k ฯ dE ฯ ฯ
k
15 cm
400, and 600K. Calculate the hole concentration and the position of the Fermi level with respect to the
intrinsic Fermi level at these temperatures. Assume that for germanium, NC =1.03x
19 cm
NV=5.35x
18 cm
Solution:
2 = ๐๐ ๐๐ด๐ค๐๐ ๏ฟฝ
and ๐ 0 =
๐๐ โ๐๐
2
๐๐ โ๐๐
2
2
2 , ๐๐ด โซ ๐๐ โ ๐ 0 =
๐๐
2
๐๐
2
2
2
10 ๐๐
โ , ๐ 0 = 1 ร 10
15 ๐๐
โ , ๐ธ๐น๐ โ ๐ธ๐น = 0.177 ๐ค๐
14 ๐๐
โ , ๐ 0 = 1.206 ร 10
15 ๐๐
โ , ๐ธ๐น๐ โ ๐ธ๐น = 0.0305 ๐ค๐
16 ๐๐
โ , ๐ 0 = 1.285 ร 10
16 ๐๐
โ , ๐ธ๐น๐ โ ๐ธ๐น = 0.00210 ๐ค๐
7 (10%) The Fermi level in n-type germanium at T=300K is 245 meV below the conduction band and 200
meV below the donor level with a donor concentration of 10
18 cm
electron (a) in the donor level and (b) in the conduction band minimum. Also calculate electron density n 0.
Solution:
(a)
For the donor level
โ
(b)
We have
โ
19 ๐๐
โ ร 7.794 ร 10
โ = 8.028 ร 10
14 ๐๐
โ