Semiconductors Principles

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Presentation transcript:

Semiconductors Principles 1

Table 2.1 Electrical Classification of Solid Materials Materials Resistivity (W-cm) Insulators 105 < r <  Semiconductors 10-3 < r < 105 Conductors r < 10-3

Table 2.3 - Semiconductor Materials Semiconductor Bandgap Energy EG (eV) Carbon (Diamond) 5.47 Silicon 1.12 Germanium 0.66 Tin 0.082 Gallium Arsenide 1.42 Indium Phosphide 1.35 Boron Nitride 7.50 Silicon Carbide 3.00 Cadmium Selenide 1.70

Diodes 19

sedr42021_0301a.jpg Figure 3.1 The ideal diode: (a) diode circuit symbol; (b) i–v characteristic; (c) equivalent circuit in the reverse direction; (d) equivalent circuit in the forward direction.

Figure 3.2 The two modes of operation of ideal diodes and the use of an external circuit to limit the forward current (a) and the reverse voltage (b). sedr42021_0302a.jpg

sedr42021_0303a.jpg Figure 3.3 (a) Rectifier circuit. (b) Input waveform. (c) Equivalent circuit when vI  0. (d) Equivalent circuit when vI  0. (e) Output waveform.

Figure E3.1 sedr42021_e0301.jpg

Figure 3.4 Circuit and waveforms for Example 3.1. sedr42021_0304a.jpg

Figure 3.5 Diode logic gates: (a) OR gate; (b) AND gate (in a positive-logic system). sedr42021_0305a.jpg

sedr42021_0306a.jpg Figure 3.6 Circuits for Example 3.2.

sedr42021_e0304a.jpg Figure E3.4

Figure 3.7 The i–v characteristic of a silicon junction diode. sedr42021_0307.jpg

sedr42021_0308.jpg Figure 3.8 The diode i–v relationship with some scales expanded and others compressed in order to reveal details.

Figure 3.9 Illustrating the temperature dependence of the diode forward characteristic. At a constant current, the voltage drop decreases by approximately 2 mV for every 1C increase in temperature. sedr42021_0309.jpg

Figure E3.9 sedr42021_e0309.jpg

Figure 3. 39 Simplified physical structure of the junction diode Figure 3.39 Simplified physical structure of the junction diode. (Actual geometries are given in Appendix A.) sedr42021_0339.jpg

sedr42021_0340.jpg Figure 3.40 Two-dimensional representation of the silicon crystal. The circles represent the inner core of silicon atoms, with +4 indicating its positive charge of +4q, which is neutralized by the charge of the four valence electrons. Observe how the covalent bonds are formed by sharing of the valence electrons. At 0 K, all bonds are intact and no free electrons are available for current conduction.

sedr42021_0341.jpg Figure 3.41 At room temperature, some of the covalent bonds are broken by thermal ionization. Each broken bond gives rise to a free electron and a hole, both of which become available for current conduction.

Figure 3.42 A bar of intrinsic silicon (a) in which the hole concentration profile shown in (b) has been created along the x-axis by some unspecified mechanism. sedr42021_0342a.jpg

sedr42021_0343.jpg Figure 3.43 A silicon crystal doped by a pentavalent element. Each dopant atom donates a free electron and is thus called a donor. The doped semiconductor becomes n type.

sedr42021_0344.jpg Figure 3.44 A silicon crystal doped with a trivalent impurity. Each dopant atom gives rise to a hole, and the semiconductor becomes p type.

sedr42021_0345a.jpg Figure 3.45 (a) The pn junction with no applied voltage (open-circuited terminals). (b) The potential distribution along an axis perpendicular to the junction.

Figure 3.46 The pn junction excited by a constant-current source I in the reverse direction. To avoid breakdown, I is kept smaller than IS. Note that the depletion layer widens and the barrier voltage increases by VR volts, which appears between the terminals as a reverse voltage. sedr42021_0346.jpg

Figure 3.47 The charge stored on either side of the depletion layer as a function of the reverse voltage VR. sedr42021_0347.jpg

Figure 3.48 The pn junction excited by a reverse-current source I, where I > IS. The junction breaks down, and a voltage VZ , with the polarity indicated, develops across the junction. sedr42021_0348.jpg

Figure 3.49 The pn junction excited by a constant-current source supplying a current I in the forward direction. The depletion layer narrows and the barrier voltage decreases by V volts, which appears as an external voltage in the forward direction. sedr42021_0349.jpg

Figure 3.50 Minority-carrier distribution in a forward-biased pn junction. It is assumed that the p region is more heavily doped than the n region; NA @ ND. sedr42021_0350.jpg

Figure 3.10 A simple circuit used to illustrate the analysis of circuits in which the diode is forward conducting. sedr42021_0310.jpg

Figure 3. 11 Graphical analysis of the circuit in Fig. 3 Figure 3.11 Graphical analysis of the circuit in Fig. 3.10 using the exponential diode model. sedr42021_0311.jpg

sedr42021_0312.jpg Figure 3.12 Approximating the diode forward characteristic with two straight lines: the piecewise-linear model.

Figure 3.13 Piecewise-linear model of the diode forward characteristic and its equivalent circuit representation. sedr42021_0313a.jpg

Figure 3. 14 The circuit of Fig. 3 Figure 3.14 The circuit of Fig. 3.10 with the diode replaced with its piecewise-linear model of Fig. 3.13. sedr42021_0314.jpg

sedr42021_0315.jpg Figure 3.15 Development of the constant-voltage-drop model of the diode forward characteristics. A vertical straight line (B) is used to approximate the fast-rising exponential. Observe that this simple model predicts VD to within 0.1 V over the current range of 0.1 mA to 10 mA.

Figure 3.16 The constant-voltage-drop model of the diode forward characteristics and its equivalent-circuit representation. sedr42021_0316a.jpg

Figure E3.12 sedr42021_e0312.jpg

Figure 3. 17 Development of the diode small-signal model Figure 3.17 Development of the diode small-signal model. Note that the numerical values shown are for a diode with n = 2. sedr42021_0317a.jpg

Figure 3. 18 (a) Circuit for Example 3. 6 Figure 3.18 (a) Circuit for Example 3.6. (b) Circuit for calculating the dc operating point. (c) Small-signal equivalent circuit. sedr42021_0318a.jpg

Figure 3.19 Circuit for Example 3.7. sedr42021_0319.jpg

sedr42021_e0316.jpg Figure E3.16

sedr42021_tb0301.jpg Table 3.1 Modeling the Diode Forward Characteristic

sedr42021_tb0307.jpg Table 3.1 (Continued)

Figure 3.20 Circuit symbol for a zener diode. sedr42021_0321.jpg Figure 3.21 The diode i–v characteristic with the breakdown region shown in some detail. Figure 3.22 Model for the zener diode.

Figure 3. 23 (a) Circuit for Example 3. 8 Figure 3.23 (a) Circuit for Example 3.8. (b) The circuit with the zener diode replaced with its equivalent circuit model. sedr42021_0323a.jpg

Figure 3.24 Block diagram of a dc power supply. sedr42021_0324.jpg

sedr42021_0325a.jpg Figure 3.25 (a) Half-wave rectifier. (b) Equivalent circuit of the half-wave rectifier with the diode replaced with its battery-plus-resistance model. (c) Transfer characteristic of the rectifier circuit. (d) Input and output waveforms, assuming that rD ! R.

sedr42021_0326a.jpg Figure 3.26 Full-wave rectifier utilizing a transformer with a center-tapped secondary winding: (a) circuit; (b) transfer characteristic assuming a constant-voltage-drop model for the diodes; (c) input and output waveforms.

sedr42021_0327a.jpg Figure 3.27 The bridge rectifier: (a) circuit; (b) input and output waveforms.

Figure 2.7 A full-wave bridge rectifier: (a) circuit showing the current direction for a positive input cycle, (b) current direction for a negative input cycle, and (c) input and output voltage waveforms

sedr42021_0328a.jpg Figure 3.28 (a) A simple circuit used to illustrate the effect of a filter capacitor. (b) Input and output waveforms assuming an ideal diode. Note that the circuit provides a dc voltage equal to the peak of the input sine wave. The circuit is therefore known as a peak rectifier or a peak detector.

sedr42021_0329a.jpg Figure 3.29 Voltage and current waveforms in the peak rectifier circuit with CR @ T. The diode is assumed ideal.

Figure 3.30 Waveforms in the full-wave peak rectifier. sedr42021_0330.jpg

Figure 3.31 The “superdiode” precision half-wave rectifier and its almost-ideal transfer characteristic. Note that when vI > 0 and the diode conducts, the op amp supplies the load current, and the source is conveniently buffered, an added advantage. Not shown are the op-amp power supplies. sedr42021_0331a.jpg

Figure 3.32 General transfer characteristic for a limiter circuit. sedr42021_0332.jpg

Figure 3.33 Applying a sine wave to a limiter can result in clipping off its two peaks. sedr42021_0333.jpg Figure 3.34 Soft limiting.

sedr42021_0335.jpg Figure 3.35 A variety of basic limiting circuits.

Figure E3.27 sedr42021_e0327.jpg

Figure 3.36 The clamped capacitor or dc restorer with a square-wave input and no load. sedr42021_0336.jpg

Figure 3.37 The clamped capacitor with a load resistance R. sedr42021_0337.jpg

sedr42021_0338a.jpg Figure 3.38 Voltage doubler: (a) circuit; (b) waveform of the voltage across D1.

Figure 3.51 The SPICE diode model. sedr42021_0351.jpg

Figure 3.52 Equivalent-circuit model used to simulate the zener diode in SPICE. Diode D1 is ideal and can be approximated in SPICE by using a very small value for n (say n = 0.01). sedr42021_0352.jpg

Figure 3. 53 Capture schematic of the 5-V dc power supply in Example 3 sedr42021_0353.jpg

Figure 3.54 The voltage vC across the smoothing capacitor C and the voltage vO across the load resistor Rload = 200  in the 5-V power supply of Example 3.10. sedr42021_0354.jpg

sedr42021_0355.jpg Figure 3.55 The output-voltage waveform from the 5-V power supply (in Example 3.10) for various load resistances: Rload = 500 , 250 , 200 , and 150 . The voltage regulation is lost at a load resistance of 150 .

Figure E3.35 (a) Capture schematic of the voltage-doubler circuit (in Exercise 3.35). sedr42021_e0335a.jpg

sedr42021_e0335b.jpg Figure E3.35 (Continued) (b) Various voltage waveforms in the voltage-doubler circuit. The top graph displays the input sine-wave voltage signal, the middle graph displays the voltage across diode D1, and the bottom graph displays the voltage that appears at the output.

sedr42021_p03002a.jpg Figure P3.2

sedr42021_p03003a.jpg Figure P3.3

sedr42021_p03004a.jpg Figure P3.4 (Continued)

sedr42021_p03004g.jpg Figure P3.4 (Continued)

sedr42021_p03005.jpg Figure P3.5

sedr42021_p03006a.jpg Figure P3.6

sedr42021_p03009a.jpg Figure P3.9

sedr42021_p03010a.jpg Figure P3.10

sedr42021_p03016.jpg Figure P3.16

sedr42021_p03023.jpg Figure P3.23

sedr42021_p03025.jpg Figure P3.25

sedr42021_p03026.jpg Figure P3.26

sedr42021_p03028.jpg Figure P3.28

sedr42021_p03054.jpg Figure P3.54

sedr42021_p03056.jpg Figure P3.56

sedr42021_p03057.jpg Figure P3.57

sedr42021_p03058.jpg Figure P3.58

sedr42021_p03059.jpg Figure P3.59

sedr42021_p03063.jpg Figure P3.63

sedr42021_p03082.jpg Figure P3.82

sedr42021_p03091.jpg Figure P3.91

sedr42021_p03092.jpg Figure P3.92

sedr42021_p03093a.jpg Figure P3.93

sedr42021_p03097.jpg Figure P3.97

sedr42021_p03098.jpg Figure P3.98

sedr42021_p03102.jpg Figure P3.102

sedr42021_p03103.jpg Figure P3.103

sedr42021_p03105.jpg Figure P3.105

sedr42021_p03108.jpg Figure P3.108