1 MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Electrical Engineering and Computer Science 6.012 MICROELECTRONIC DEVICES AND CIRCUITS Problem Set No. 5 Issued: October 7, 2009 Due: October 14, 2009 Reading Assignments: Lecture 9 (10/8/09) - Chap. 9 (9.1, 9.2, 9.3, 9.4) Lecture 10 (10/15/09) - Chap. 9 (9.3, 9.4) Lecture 11 (10/20/09) - Chap. 10 (10.1.1a) Problem 1 - Two short MOS capacitor problems from the textbook: a) Do Problem 9.1 in the course text, Parts a, b, c, and d, only. In Part d) ii) use the value 1000 cm2/V-s for the electron mobility. b) Do Problem 9.8 in the course text. A MOSFET connected as it is in this question is simply a MOS capacitor. Problem 2 – We have only plotted the net sheet charge densities and the electrostatic potential through the MOS capacitors we have discussed, but we have not said anything about the electric field. To address this issue, sketch and label the electric fieldthrough an MOS capacitor for biases corresponding to the five conditions illustrated inFigure 9.3 (parts a thru f) on pages 244 and 245 in the course text. That is, make theelectric field sketches that correspond to this set of charge density and electrostaticpotential plots. Problem 3 – Consider the two silicon device structures shown in cross-section below: Device A: Device B: n+p-Si15 µm5 µm GBn+p-SiG20 µmBBoth of these devices are made on p-type silicon with a net doping level of 1017 cm-3, and are 20 µm wide normal to the page. The n+ regions are doped to 1018 cm-3, and the n+-p junction is 1 µm from the top surface. The thin oxide is a high quality2 thermal oxide 16 nm thick, and covers an area 20 µm wide by 15 µm long. In Device A the n+ region is 20 µm wide by 5 µm long and extends just up to the edge of the thin oxide, while in Device B it is 20 µm wide by 20 µm long and extends all the way underthe thin oxide, as shown in the figure. You may assume that throughout the silicon the electron mobility, µe, is 1600 cm2/V-s and the hole mobility, µh, is 600 cm2/V-s (except in an inversion layer in which case µe = 600 cm2/V-s and µh = 400 cm2/V-s); that the intrinsic carrier concentration, ni, is 1010 cm-3 at room temperature; and that the dielectric constant, εSi, is 10-12 F/cm. The dielectric constant of the oxide, εox, is 3 x 10-13 F/cm, and the electrostatic potential of the gate metal relative to intrinsic Si is 0.3 V. (Note: There is more information here than you need.) a) i) What is the electrostatic potential of the p-type silicon, relative to intrinisicsilicon, in thermal equilibrium at room temperature? ii) What is the built-in potential of the unbiased n+-p junction at room temperature? b) What are the flat band voltages, VFB, of the MOS capacitor structures in Devices A and B, respectively? c ) The magnitude of the threshold voltage, |VT|, for the MOS structure is 1 V in one of these devices, and 4 V in the other. Use this information and your knowledge of MOS capacitors to deduce the magnitude and sign of VT for each of these MOS capacitors, i.e., the one made on p-Si and the made on n+-Si. d) What is the condition (accumulated, depleted, or inverted) of the semiconductorsurface under the thin oxide in each of these devices with a gate voltage, VGB, of 2 Volts? Also give the identity and sheet density of any mobile holes or electrons induced at the oxide-silicon interface. Problem 4 - This problem concerns the novel semiconductor-oxide-semiconductor (SOS) structure illustrated at the top of the next page. The two semiconductor regions are both p-type silicon with a net acceptor concentration of 1016 cm-3; the oxide is a 50 nm (5 x 10-6 cm) thick layer of silicon dioxide. The dielectric constant of silicon, εSi, is 10-12 F/cm and of silicon dioxide, εox, is 3.5 x 10-13 F/cm. Use the depletion approximation model when solving this problem. Assume that the depletion region widths are less than w/2. The drawing may not be to scale. p-Si 1016 cm -3 BA -w SiO2p-Si 1016 cm -3 w-tox/2 0 tox/2 x a) Sketch and label the electrostatic potential, φ(x), in this structure between -w/2 and +w/2 when vAB = 0 and the structure is in thermal equilibrium.3 b) A bias is applied to this device sufficient to make the electrostatic potential at x = tox/2 equal to -φp, where φp is the thermal equilibrium electrostatic potential in the p-type regions, i.e., φ(tox/2) = -φp. We call this the onset of inversion on the right side, and name this bias the right-side threshold, VTR. (i) What is the sign of VTR? Explain your answer. (ii) What is the width of the depletion region to the right of x = tox/2 with this applied bias? (iii) What is the condition of the left-hand semiconductor-oxide interface, the one at x = -tox/2 with this applied bias? (iv) What is the value of VTR? c) Sketch and label the net charge density, ρ(x), for -w/2 < x < w/2 when the bias voltage, VAB, is VTR + 2 Volts; recall VTR was defined in Part (b). Be sure to label the vertical axis and to indicate the magnitude of any impulses (i.e., sheet chargedensities). d) Define the left-hand threshold, VTL, of the structure as the bias voltage, VAB, at which the potential at x = - tox/2 is -φp. What is VTL? (You can give your answer in terms of VTR, if you wish. Making use of the mirror symmetry of the structureshould simplify your calculation.) e) Consider now a different SOS structure in which the left-hand semiconductor region is doped n-type, rather than p-type, with a net donor concentration of 1016 cm-3. (i) Sketch the electrostatic potential, φ(x) for -w/2 < x < w/2 in thermal equilibrium, i.e., vAB = 0. Label the vertical axes but you do not calculate the widths of any depletion regions. (ii) Sketch and label the electrostatic potential when vAB is VTR for this new structure, where VTR has the same definition as before [see Part (b) above], but will not necessarily have the same value. (iii) What is the value of VTL for this new structure in terms of VTR for this new structure, where VTR and VTL have the same definitions as earlier? (Making use of the inversion symmetry of the problem will simplify your solution.)MIT OpenCourseWarehttp://ocw.mit.edu 6.012
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