5
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 A E n x x g 0 0 1 (1) where is in cm -1 , E g is in eV and x=h/E g . Evaluate A 0 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 E g , kT, n 0 and E p . This is called intrinsic carrier concentration n i . (b) Evaluate n i for InSb (E g =0.18 eV), GaAs (E g =1.42 eV) and ZnSe (E g =2.6 eV) at room temperature (T=300K). Take E p 21 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 k Ek Ek E p k m m m (a) Show that 2 2 2 2 2 2 2 0 0 2 4 . () () 1 1 p cv c v g g g g kE kp E k E k E E mE mE for k||p cv (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..

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

  • Upload
    others

  • View
    0

  • Download
    0

Embed Size (px)

Citation preview

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

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
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
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
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