Semiconductor Fundamentals

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Presentation transcript:

Semiconductor Fundamentals Chapter 19 Semiconductor Fundamentals

Objectives After completing this chapter, you will be able to: Identify materials that act as semiconductors Define covalent bonding Describe the doping process for creating N- and P-type semiconductor materials Explain how doping supports current flow in a semi-conductor material

Semiconduction in Germanium and Silicon Semiconductor materials Possess characteristics that fall between those of insulators and conductors Pure semiconductor elements Carbon (C) Germanium (Ge) Silicon (Si) Used for most semiconductor devices

Semiconduction in Germanium and Silicon (cont’d.) Figure 19-1. Atomic structure of silicon.

Figure 19-3. Crystalline structure of silicon with covalent bonding.

Semiconduction in Germanium and Silicon (cont’d.) Negative temperature coefficient As temperature increases, resistance decreases Heat Potential source of trouble for semiconductors Electrons break their covalent bonds

Figure 19-4. A hole is created when an electron breaks its covalent bond.

Conduction in Pure Germanium and Silicon (cont’d.) Figure 19-5. Current flow in pure semiconductor material.

Conduction in Doped Germanium and Silicon Doping Adding impurities to a semiconductor material Pentavalent Made of atoms with five valence electrons Trivalent Made of atoms with three valence electrons

Conduction in Doped Germanium and Silicon (cont’d.) N-type material Pentavalent materials Electrons are the majority carrier Holes are the minority carrier

Figure 19-6. Silicon semiconductor material doped with an arsenic atom.

Conduction in Doped Germanium and Silicon (cont’d.) Figure 19-7. Current flow in N-type material.

Conduction in Doped Germanium and Silicon (cont’d.) P-type material Trivalent materials Holes are the majority carrier Electrons are the minority carrier

Figure 19-8. Silicon semiconductor material doped with an indium atom.

Conduction in Doped Germanium and Silicon (cont’d.) Figure 19-9. Current flow in P-type material.

Summary Pure semiconductor materials are germanium, silicon, and carbon As the temperature increases in a semiconductor material, electrons drift from one atom to another Current flow in semiconductor materials consists of both electron flow and hole movement

Summary (cont’d.) Doping is the process of adding impurities to a semiconductor material In N-type material, electrons are the majority carrier and holes are the minority carrier In P-type material, holes are the majority carrier and electrons are the minority carrier