phyc 569, advanced topics in modern optics fall 2016 ...22g cv kk e k e k e p k m m m (a) show that...
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![Page 1: PHYC 569, Advanced Topics in Modern Optics Fall 2016 ...22g cv kk E k E k E p k m m m (a) Show that 2 2 22 2 2 2 00 4. 2 ( ) ( ) 1 1cv p c v g g gg kp kE E k E k E E m E m E for k||p](https://reader034.vdocument.in/reader034/viewer/2022050601/5fa902fe8b013201b94f777c/html5/thumbnails/1.jpg)
PHYC 569, Advanced Topics in Modern Optics (Laser Physics II: PHYC/ECE 564)
Fall 2016
Homework #2, Due Tuesday Sept. 20
Instructor: M. Sheik-Bahae
1. Show that the interband absorption coefficient of semiconductors can be given as:
( )h AE
n
x
x
g
0
0
1 (1)
where is in cm-1
, Eg is in eV and x=h/Eg. Evaluate A0 in the effective mass approximation.
2. (a) Derive the formula for thermally-ionized electron-hole concentration in an intrinsic (i.e.
undoped) semiconductor in terms of Eg, kT, n0 and Ep. This is called intrinsic carrier
concentration ni.
(b) Evaluate ni for InSb (Eg=0.18 eV), GaAs (Eg=1.42 eV) and ZnSe (Eg=2.6 eV) at room
temperature (T=300K). Take Ep21 eV for all semiconductors.
3. Strictly speaking, the energy-momentum dispersion relation for a two band (c and v)
system is not purely parabolic and is given by the equation (e.g. see S. L. Chuang, 4.1.16):
2 2 2 2 2
2
2
0 0 0
( ) . ( ) | |2 2
g cv
k kE k E k E p k
m m m
(a) Show that
2 2 22
2 2 2
0 0
24 .( ) ( ) 1 1
pcv
c v g g
g g
k Ek pE k E k E E
m E m E for k||pcv (light holes)
(b) Calculate the joint density of state cv(E), and the absorption coefficient 0(h) for such
non-parabolic bands. Compare your result with that given by Eq.(1) by plotting the two
absorption coefficients versus photon energy..
![Page 2: PHYC 569, Advanced Topics in Modern Optics Fall 2016 ...22g cv kk E k E k E p k m m m (a) Show that 2 2 22 2 2 2 00 4. 2 ( ) ( ) 1 1cv p c v g g gg kp kE E k E k E E m E m E for k||p](https://reader034.vdocument.in/reader034/viewer/2022050601/5fa902fe8b013201b94f777c/html5/thumbnails/2.jpg)
![Page 3: PHYC 569, Advanced Topics in Modern Optics Fall 2016 ...22g cv kk E k E k E p k m m m (a) Show that 2 2 22 2 2 2 00 4. 2 ( ) ( ) 1 1cv p c v g g gg kp kE E k E k E E m E m E for k||p](https://reader034.vdocument.in/reader034/viewer/2022050601/5fa902fe8b013201b94f777c/html5/thumbnails/3.jpg)
![Page 4: PHYC 569, Advanced Topics in Modern Optics Fall 2016 ...22g cv kk E k E k E p k m m m (a) Show that 2 2 22 2 2 2 00 4. 2 ( ) ( ) 1 1cv p c v g g gg kp kE E k E k E E m E m E for k||p](https://reader034.vdocument.in/reader034/viewer/2022050601/5fa902fe8b013201b94f777c/html5/thumbnails/4.jpg)
![Page 5: PHYC 569, Advanced Topics in Modern Optics Fall 2016 ...22g cv kk E k E k E p k m m m (a) Show that 2 2 22 2 2 2 00 4. 2 ( ) ( ) 1 1cv p c v g g gg kp kE E k E k E E m E m E for k||p](https://reader034.vdocument.in/reader034/viewer/2022050601/5fa902fe8b013201b94f777c/html5/thumbnails/5.jpg)