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8/22/2019 Set 7 Web Solutions LC
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P3000 LON-CAPA Set 7 Sample Solutions
1. pn Junction: From Neamen Sect. 9.2. Calculate the magnitude of the applied reverse-
bias voltage at which the ideal reverse current in a pn junction diode at T = 290 K reaches
81 % of its reverse saturation value. Enter your answer in volts.
Cor r ect , comput er get s: 4. 15e- 02
Hint:
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2. pn Junction: From Neamen Sect. 9.2. Consider an ideal silicon pn junction diode
with the following parameters: tau_n0 = 1.0010-7
s, tau_p0 = 1.0010-7
s, D_n = 30cm^2/s, and D_p=12 cm^2/s. What ratio of acceptor concentration (N_a) to donor
concentration (N_d), is needed so that 55 % of the depletion curent is carried by
electrons? Enter your answer as the value of N_a/N_d.
Corr ect , computer get s: 1. 29e+00
Hint:
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3. Optical Absorption: From Neamen Sect. 12.1. Calculate the maximum wavelength
of a light source that can generate electron-hole pairs in GaAs. Enter your answer in cm.
Cor r ect , comput er get s: 8. 71e- 05
4. Optical Absorption: From Neamen Sect. 12.1. Photons of energy 1.34 eV are incident
on a thin slab of silicon at a power density (intensity) of 1.0010-2
W/cm^2. Theabsorption coefficient for silicon at this photon energy is 1.5210
2cm^-1. The excess
minority-carrier lifetime is 1.0010-6
s. In the first box, enter the electon-hole generation
rate in units of cm^-3*s^-1. In the second box, enter the steady-state excess carrierconcentration in cm^-3. Neglect surface effects.
Corr ect , comput er get s: 7. 09e+18, 7. 09e+12
Hint: Be very careful with units!
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5. Optical Absorption: From Neamen Sect. 12.1. Photons of energy 1.67 eV are incident
on a slab of GaAs. The absorption coefficient for GaAs at this photon energy is 1.70104
cm^-1. In the first box, enter the thickness, in cm, of GaAs so that 65 % of the energy is
absorbed. In the second box, enter the thickness, in cm, of GaAs so that 65 % of the
energy is transmitted.
Cor r ect , comput er get s: 6. 18e- 05, 2. 53e- 05
Hint: Be very careful with units!
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6. Solar Cells: From Neamen Sect. 12.2. Consider an ideal long n^+p junction GaAs
solar cell at T = 300 K in which excess carriers are uniformly generated. The parametersof the diode area as follows: N_d = 1.2010
19cm^-3, tau_n0 = 5.0010
-8s, tau_p0 =
5.0010-8
s, D_n=225 cm^2/s, D_p = 7 cm^2/s. The generated photcurrent density is J_L
= 31 mA/cm^2. In the first box, enter the reverse saturation current for this diode, in
A/cm^2, assuming that the acceptor concentration density on the p side is 1.0010
16
cm^-3. In the second box, enter the corresponding open-circuit voltage in volts. In the
calculation of minority carrier concentrations, you may use the intrinsic carrier
concentration for GaAs provided in table B4 of your text book.
Cor r ect , comput er get s: 3. 48e- 18, 9. 50e- 01
Hint: You can find an expression for the reverse saturation current of a pn diode in
section 9.2 of your text.
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7. Photodectectors: From Neamen Sect. 12.2. Repeat the previous question assuming an
acceptor concentration density on the p side is 7.001018
cm^-3. In the first box, enter thereverse saturation current in A/cm^2. In the second box, enter the corresponding open-
circuit voltage in volts.
Corr ect , computer gets: 5. 48e- 21, 1. 12e+00
Hint: You can find an expression for the reverse saturation current of a pn diode in
section 9.2 of your text.
8. LEDs From Neamen Sect. 12.3. Consider a silicon PIN diode at T = 300 K illuminated
by an incident photon flux of Phi_0 = 4.001017
cm^-2*s^-1. Assume that the width ofthe intrinsic layer is 1.0010
-2cm. Enter the prompt photocurrent density in A/cm^2.
Assume that the absorption coefficient is 3.00103 cm^-1.
Cor r ect , comput er get s: 6. 40e- 02
Hint: Be careful with units!
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9. [4pt] From Neamen Sect. 12.4. Consider a pn junction GaAs LED. Assume that
photons are generated uniformly in all directions on a plane to the junction at a distanceof 0.50e-6 m fom the surface. In the first box, enter the fraction, as a percentage, of the
emitted photons that have the potential of being emitted from the semiconductor surface
without undergoing total internal reflection. In the second box, enter the fraction, as a
percentage, of generated photons that can be emitted into air when both total internalreflection and Fresnel loss are taken into account. Neglect absorption losses. Assume that
the index of refraction for GaAs is 3.66.
Cor r ect , comput er get s: 8. 81, 5. 94
Hint: For the total internal reflection part, remember that the problem says that the
photons are emitted in all directions along a plane, not in all directions in 3 dimensions.
For the second part, that the Fresnell loss will be on top of the losses due to total internalreflection.