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SOLUTIONS MANUAL for Dopants and Defects in Semiconductors 2nd Edition by Matthew McCluskey, Eugene Haller and Eugene Haller | All Chapters 1-12 $32.48   Add to cart
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SOLUTIONS MANUAL for Dopants and Defects in Semiconductors 2nd Edition by Matthew McCluskey, Eugene Haller and Eugene Haller | All Chapters 1-12
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SOLUTIONS MANUAL for Dopants and Defects in Semiconductors 2nd Edition by Matthew McCluskey, Eugene Haller and Eugene Haller ISBN 9781351977975 (All Chapters 1-12)

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  • November 30, 2023
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  • 2023/2024
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  • dopants and defects in semiconductors 2nd edition
  • dopants and defects in semiconductors
  • solutions manual for dopants and defects in semico
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, Dopants and Defects in Semiconductors
Second Edition


Matthew D. McCluskey and Eugene E. Haller




Solutions Manual




*Corrections or comments may be sent to mattmcc@alum.mit.edu


1

,Chapter 1


1.1 Silicon density = 2.33 g/cm3.
1 mole = 28 g
(2.33 g/cm3)(1 mole / 28 g)(6.02×1023 / mole) = 5×1022 cm-3
8/a3 = 5×1022 cm-3
a = 5.5×10-8 cm = 5.5 Å
2 3
d  a 2 42  a 2 4  a 2 42  a = 2.39 Å
4


1.2 Germanium a = 5.66 Å = 5.66×10-8 cm.
Density = 8/a3 = 4.4×1022 cm-3


1.3 Strontium titanate (SrTiO3) has the perovskite structure.
(a) Unit cube with the atoms:




(b) Each Ti atom is bonded to 6 O atoms.
(c) Molecular mass = 183.49u
a = 3.9 Å
Number density = 1/a3 = 1.69×1022 cm-3
(1.69×1022 / cm3)(183.49 g / mole)(1 mole / 6.02×1023) = 5.14 g/cm3


1.4 Plot E versus kx along the [100] direction, up to a maximum energy of 52π2/2ma2.




2

,  2  2  
2 2 2
2   2  
E  k x  nx    k y  ny    kz  nz  
2m  a   a   a  

2 2
1. nx = ny = nz = 0, E  kx
2m

2 2  22
2. nx = 0, ny or nz = ±1, E  kx  4
2m 2ma 2
2
2  2 
3. nx = ±1, ny = nz = 0, E kx  
2m  a 




1.5 An intrinsic semiconductor has no defects, or few enough to not affect its properties
significantly. An extrinsic semiconductor’s properties are determined by defects.



1.6 f E   E  E  / kT
1 1
 4.0 = 0.018
e F
1 e 1



1.7 The effective mass is the largest for the heavy-hole band.




3

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