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Electronics Electronics Principles & Applications Principles & Applications Fifth Edition Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

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Page 1: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

ElectronicsElectronics

Principles & ApplicationsPrinciples & ApplicationsFifth EditionFifth Edition

Chapter 2Semiconductors

©1999 Glencoe/McGraw-Hill

Charles A. Schuler

Page 2: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

• Conductors and Insulators• Semiconductors• N-type Semiconductors• P-type Semiconductors• Majority and Minority Carriers

INTRODUCTION

Page 3: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

NN

NN

The center of an atom is called the nucleus.Most atoms have neutrons which have no charge.A nucleus also has protonsand they have a positive charge.

Negative electronsorbit the nucleus.

Page 4: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

NN

NN

This is a copper atom.

It has 29 protons.

It has 29 electrons.

Its net charge = 0.

Valence electron

Page 5: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

The valence electron is the important feature.

NN

NN

Valence electron

Its attraction to the nucleus is relatively weak.

Page 6: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

The valence electron

The nucleus plus the inner electron orbits

A simple model of the copper atom looks like this:

Page 7: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Copper wire is usedto conduct electricitybecause the valence

electrons move freelythrough its structure.

Remember, the valenceelectrons are weakly

attracted to the nuclei.

Page 8: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

So far, we know that copper’s single valence electron makes it a good conductor.

It acts as an electrical insulator.

The rule of eight states that a material like thiswould be stable since its valence orbit is full.

No Vacancy

Page 9: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Atomic quiz

The dense and central part of any atom iscalled the ________. nucleus

Atom net charge is 0 since the number of protonsequals the number of ______. electrons

The outermost orbit of all atoms is calledthe ________ orbit. valence

Good electrical conductors have freevalence ________. electrons

The magic number for valence stabilityis ________. eight

Page 10: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Atoms of the same type can join together and form covalent bonds.

This is an electron sharing process.

Silicon atoms have four valence electrons.

Page 11: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

The covalent sharing satisfies the rule of eight.

In this structure, one bond is formed with each neighbor

Page 12: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

This is a silicon crystal.

It does not conduct because its valence electrons are held by covalent bonds.

Page 13: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Thermal carriers

Covalent bonds can be broken by heating a silicon crystal.

Free electron

Hole

Page 14: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

The thermal carriers support the flow of current.

Page 15: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Heating silicon crystals to make them conduct is not practical!

Page 16: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

This is an arsenic atom.

A silicon crystal can be doped with a donor impurity.

1

2 3

45

Each donor atom that enters the crystal adds a free electron.

Free electron

Page 17: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Silicon that has been doped with arsenic is called N-type.

The free electrons in N-type silicon support the flow of current.

Page 18: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

This is a boron atom.

A silicon crystal can be doped with an acceptor impurity.

1

2 3Each acceptor atom that enters the crystal creates a hole.

Hole

Page 19: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Silicon that has been doped with boron is called P-type.

The holes in P-type silicon support the flow of current.

Page 20: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

What are two practical methodsof making silicon semiconduct?

HoleFree electron

Add a pentavalentimpurity

Add a trivalentimpurity

(N type) (P type)

Page 21: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

This is a P-type crystal.

Due to heat, it could have a few free electrons.

These are called minority carriers.

Page 22: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

This is an N-type crystal.

Due to heat, it could have a few free holes.

These are called minority carriers.

Page 23: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

Semiconductor quiz

A pure silicon crystal, at room temperature,acts as an electrical ________. insulator

The current carriers, in N-type silicon, arecalled ________. electrons

The current carriers, in P-type silicon, arecalled ________. holes

The minority carriers, in N-type silicon, arecalled ________. holes

The minority carriers, in P-type silicon, arecalled ________. electrons

Page 24: Electronics Principles & Applications Fifth Edition Chapter 2 Semiconductors ©1999 Glencoe/McGraw-Hill Charles A. Schuler

REVIEW

• Conductors and Insulators• Semiconductors• N-type Semiconductors• P-type Semiconductors• Majority and Minority Carriers