Homework 3 Problem 1: Sze Chapter 2, #20, pg. 133 Problem 2 ...
Homework 3 Problem 1: Sze Chapter 2, #20, pg. 133 Problem 2 ...
Homework 3 Problem 1: Sze Chapter 2, #20, pg. 133 Problem 2 ...
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SDM II<br />
Fall 2010<br />
<strong>Problem</strong> 1:<br />
<strong>Sze</strong> <strong>Chapter</strong> 2, <strong>#20</strong>, <strong>pg</strong>. <strong>133</strong><br />
<strong>Homework</strong> 3<br />
The alignment of heterojunction between GaAs and Al 0.4Ga0.6As is Type-I. The conduction-band<br />
discontinuity is Ec=0.28 eV. The doping concentration is 1020 cm-3 in Al0.4Ga0.6As and 1016 cm-3 in GaAs, both doped with carbon.<br />
(a) Find the total depletion width under thermal equilibrium condition, assuming the dielectric<br />
constant is the same for both semiconductors<br />
(b) Draw the band diagram for V=0<br />
<strong>Problem</strong> 2:<br />
<strong>Sze</strong> <strong>Chapter</strong> 2, #18, <strong>pg</strong>. 132<br />
Prof. Shayla Sawyer<br />
<strong>Homework</strong> 3<br />
Consider an ideal abrupt heterojunction with a built-in potential of 1.6V. The impurity concentrations in semiconductor 1<br />
and 2 are 1x10 16 donors/cm 3 and 3x10 19 acceptors/cm 3, and dielectric constants are 12 and 13, respectively. Find the<br />
electrostatic potential and depletion width in each material for applied voltages of 0.5V and -5V.<br />
<strong>Problem</strong> 3:<br />
<strong>Sze</strong> <strong>Chapter</strong> 8, #5, <strong>pg</strong>. 464<br />
Molecular beam epitaxy interfaces are typically abrupt to within on eor two monolayers (one monolayer ~ 2.8 Å in GaInAs),<br />
due to terrace formation in the growth plane. Estimate the energy level broadening for the ground and first excited<br />
electron states of a 15-nm GaInAs quantum well bound by thinck AlInAs barriers. (Hint: Assume the case of two<br />
monolayer thickness fluctiaotn and an infinite deep QW. The electron effective mass in GaInAs is 0.0427m o .<br />
<strong>Problem</strong> 4:<br />
<strong>Sze</strong> <strong>Chapter</strong> 7, #10, <strong>pg</strong>. 413<br />
(a) Find the threshold voltages of a conventional and a delta-doped heterostructure AlGaAs-GaAs FETs<br />
(b) Evaluate the variations of these threshold voltages for two-monolayer fluctuations in AlGaAs layer thickness.<br />
Assuming that one monolayer = 3 Å in AlGaAs, the Schottky barrier height is 0.9V, the conduction-band discontinuity is<br />
0.3eV, the uniform doping in the conventional HFET is 10 18 cm-3 with a thickness of 40 nm, the delta doping is located 40<br />
nm from the metal-semiconductor interface, with a sheet charge density of 1.5 x 10 12 cm-2, and the dielectric permittivity<br />
for AlGaAs is assumed to be 10-12 F/cm.<br />
Bonus, <strong>Problem</strong> 5:<br />
NanoHub (H-S. Philip Wong)<br />
Use software on nanoHUB.org to plot the I-V characteristics of a resonant tunneling diode. In this problem, we will use software on nanoHUB.org to plot<br />
the I-V characteristic of a resonant tunneling diode. Visit the following page:<br />
http://nanohub.org/tools/rtd<br />
Please use the following parameters:<br />
a) 2-barrier device<br />
b) Barrier thickness (Al0.3Ga0.7As): 5nm<br />
c) Well thickness (GaAs): 5 nm<br />
d) Temperature: 300 K<br />
e) Doping at contacts: 1018 /cm3 Plot the I-V characteristic for V=0 ~ 0.4 volt. What are the values of Ip & Iv? MORE BELOW!
SDM II<br />
Fall 2010<br />
p.s. DON'T turn the self-consistent potential on<br />
2.Design a RTD that gives the largest PVCR (peak-to-valley current ratio). You can adjust any parameter in the simulator, and again, DON'T turn on<br />
the self-consistent analysis.<br />
Explain why and how you choose your parameters to maximize the PVCR.<br />
Prof. Shayla Sawyer<br />
<strong>Homework</strong> 3