Microelectronics Tech: ECSE-2210 Homework Solutions - Carrier Concentration, Assignments of Electrical and Electronics Engineering

The solutions to homework 2 of the microelectronics technology course (ecse-2210) at a specific university. It covers calculations related to carrier concentrations (electron density, hole density, and intrinsic carrier density) at various temperatures. Students can use this document to check their understanding of the concepts and equations presented in the course.

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Pre 2010

Uploaded on 08/09/2009

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ECSE-2210 Microelectronics Technology
Homework 2 – Solution
1. Always, n p ni 2
At 300 K, n = 1017 cm–3, ni = 1010 cm–3, p = 103 cm–3
At 200 K, n = 1017 cm–3, ni = 105 cm–3, p = 10-7 cm–3
That is, the hole concentration at 200 K is extremely small. You will find only one hole in a
volume of 107 cm3 of Si !
2. a) At room temperature in Si, ni = 1010 cm-3. Thus here ND >> NA , ND >> ni and
n = ND = 1015 cm–3
p = ni 2/ ND = 105 cm–3
b) Since ND << NA, NA >> ni
p = NA = 1016 cm–3
n = ni 2/ NA = 104 cm–3
c) Here we must retain both ND and NA, but ND-NA >> ni
n = ND NA = 1015 cm–3
p = ni 2/ (ND NA) = 105 cm–3
d) We deduce from Figure 2.20 that, at 450 K, ni (Si) 5 × 1013 cm–3. Clearly, ni is
comparable to ND and we must use Eq. 2.29a
n = ND /2 + [ (ND /2) + ni 2] 1/2 = 1.21 × 1014 cm–3
p = ni 2 /n = 2.07 × 1013 cm–3
e) We conclude from figure 2.20, that at 650 K, ni = 1016 cm–3 Here ni >> ND
p = ni = 1016 cm–3
n = ni = 1016 cm–3
pf2

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ECSE-2210 Microelectronics Technology Homework 2 – Solution

  1. Always, n pn i 2

At 300 K, n = 10 17 cm–3^ , n i = 10 10 cm–3^ , p = 10 3 cm–

At 200 K, n = 10 17 cm–3^ , n i = 10 5 cm–3^ , p = 10 -7^ cm–

That is, the hole concentration at 200 K is extremely small. You will find only one hole in a volume of 10^7 cm^3 of Si!

  1. a) At room temperature in Si, n i = 10 10 cm-3^. Thus here N D >> N A , N D >> n i and

n = N D = 1015 cm–

p = n i 2 / N D = 10^5 cm–

b) Since N D << N A, N A >> n i

p = N A = 1016 cm–

n = n i 2 / N A = 10 4 cm–

c) Here we must retain both N D and N A, but N D- N A >> n i

n = N D – N A = 1015 cm–

p = n i 2 / ( N D – N A) = 10 5 cm–

d) We deduce from Figure 2.20 that, at 450 K, n i (Si) ≈ 5 × 10 13 cm–3^. Clearly, n i is comparable to N D and we must use Eq. 2.29a

n = N D /2 + [ ( N D /2) + n i 2 ] 1/2^ = 1.21 × 10^14 cm–

p = n i 2 / n = 2.07 × 10^13 cm–

e) We conclude from figure 2.20, that at 650 K, n i = 10 16 cm–3^ Here n i >> N D

p = n i = 1016 cm–

n = n i = 10^16 cm–