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Callister - An introduction - 8th edition

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Summary • 769<br />

• With these materials, in addition to free electrons, holes (missing electrons in the<br />

valence band) may also participate in the conduction process (Figure 18.11).<br />

• Semiconductors are classified as either intrinsic or extrinsic.<br />

For intrinsic behavior, the electrical properties are inherent in the pure material,<br />

and electron and hole concentrations are equal. The electrical conductivity<br />

may be computed using Equation 18.13 (or Equation 18.15).<br />

Electrical behavior is dictated by impurities for extrinsic semiconductors.<br />

Extrinsic semiconductors may be either n- or p-type depending on whether<br />

electrons or holes, respectively, are the predominant charge carriers.<br />

• Donor impurities introduce excess electrons (Figures 18.12 and 18.13); acceptor<br />

impurities introduce excess holes (Figures 18.14 and 18.15).<br />

• The electrical conductivity on an n-type semiconductor may be calculated using<br />

Equation 18.16; for p-type, Equation 18.17 is employed.<br />

The Temperature Dependence of Carrier Concentration<br />

Factors That Affect Carrier Mobility<br />

• With rising temperature, intrinsic carrier concentration increases dramatically<br />

(Figure 18.16).<br />

• For extrinsic semiconductors, on a plot of majority carrier concentration versus<br />

temperature, carrier concentration is independent of temperature in the “extrinsic<br />

region” (Figure 18.17). The magnitude of carrier concentration in this region<br />

is approximately equal to the impurity level.<br />

• For extrinsic semiconductors, electron and hole mobilities (1) decrease as impurity<br />

content increases (Figure 18.18), and (2) in general, decrease with rising temperature<br />

(Figures 18.19a and 18.19b).<br />

The Hall Effect<br />

• Using a Hall effect experiment, it is possible to determine the charge carrier type<br />

(i.e., electron or hole), as well as carrier concentration and mobility.<br />

Semiconductor Devices<br />

• A number of semiconducting devices employ the unique electrical characteristics<br />

of these materials to perform specific electronic functions.<br />

• The p–n rectifying junction (Figure 18.21) is used to transform alternating current<br />

to direct current.<br />

• <strong>An</strong>other type of semiconductor device is the transistor, which may be used for amplification<br />

of electrical signals, as well as for switching devices in computer circuitries.<br />

Junction and MOSFET transistors (Figures 18.24, 18.25, and 18.26) are possible.<br />

Electrical Conduction in Ionic Ceramics and Polymers<br />

• Most ionic ceramics and polymers are insulators at room temperature. Electrical<br />

conductivities range between about 10 9 and 10 18 (#<br />

m) 1 ; by way of comparison,<br />

for most metals is on the order of 10 7 (#<br />

m) 1 .<br />

Dielectric Behavior<br />

Capacitance<br />

Field Vectors and Polarization<br />

• A dipole is said to exist when there is a net spatial separation of positively and<br />

negatively charged entities on an atomic or molecular level.<br />

• Polarization is the alignment of electric dipoles with an electric field.<br />

• Dielectric materials are electrical insulators that may be polarized when an electric<br />

field is present.

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