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Solid State Physics 3. Section 10-4,6. Topics. Heat Capacity of Electron Gas Band Theory of Solids Conductors, Insulators and Semiconductors Summary. Special Extra Credit. As can be seen from the graph, the prediction . fails at very low temperatures. This is due, in part, to the

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solid state physics 3

Solid State Physics3

Section 10-4,6

topics
Topics
  • Heat Capacity of Electron Gas
  • Band Theory of Solids
  • Conductors, Insulators and Semiconductors
  • Summary
special extra credit
Special Extra Credit

As can be seen from the

graph, the prediction

fails at very low

temperatures. This is

due, in part, to the

failure of the

equipartition theorem

at low temperatures.

Challenge: create a

better model!

special extra credit4
Special Extra Credit

Derive the temperature

dependence of R/R0 by

computing the average potential energy <E>

of a lattice ion

assuming that the energy

level of the nth

vibrational state is

rather than En = ne as

Einstein had assumed

Due:

before classes end

heat capacity of electron gas
Heat Capacity of Electron Gas

By definition, the heat capacity (at constant

volume) of the electron gas is given by

where U is the total energy of the gas. For a gas

of N electrons, each with average energy <E>,

the total energy is given by

heat capacity of electron gas6
Heat Capacity of Electron Gas

Total energy

In general, this integral must be done

numerically. However, for T << TF, we can use

a reasonable approximation.

heat capacity of electron gas7
Heat Capacity of Electron Gas

At T= 0, the total energy of the electron gas is

For 0 < T << TF, only a small fraction kT/EF

of the electrons can be excited to higher energy

states

Moreover, the energy of

each is increased by

roughly kT

heat capacity of electron gas8
Heat Capacity of Electron Gas

Therefore, the total energy can be written as

where a = p2/4, as first shown by Sommerfeld

The heat capacity of the

electron gas is predicted to

be

heat capacity of electron gas9
Heat Capacity of Electron Gas

Consider 1 mole of copper. In this case Nk = R

For copper, TF = 89,000 K. Therefore, even at

room temperature, T = 300 K, the contribution

of the electron gas to the

heat capacity of copper is

small:

CV = 0.018 R

band theory of solids
Band Theory of Solids

So far we have neglected the lattice of positively charged ions

Moreover, we have ignored the Coulomb repulsion between the electrons and the attraction between the lattice and the electrons

The band theory of solids takes into account the interaction between the electrons and the lattice ions

band theory of solids11
Band Theory of Solids

Consider the potential energy of a

1-dimensional solid

which we approximate by the Kronig-Penney Model

band theory of solids12
Band Theory of Solids

The task is to compute the quantum states and

associated energy levels of this simplified model

by solving the Schrödinger equation

1

2

3

band theory of solids13
Band Theory of Solids

For periodic potentials, Felix Bloch showed that

the solution of the Schrödinger equation must

be of the form

and the wavefunction must

reflect the periodicity of

the lattice:

1

2

3

band theory of solids14
Band Theory of Solids

By requiring the wavefunction and its derivative

to be continuous everywhere, one finds energy

levels that are grouped into bands separated by

energy gaps. The gaps occur at

The energy gaps

are basically energy

levels that cannot

occur in the solid

1

2

3

band theory of solids15
Band Theory of Solids

Completely free

electron

electron in a

lattice

band theory of solids16
Band Theory of Solids

When, the wavefunctions become

standing waves. One wave peaks at the lattice

sites, and another peaks between them. Ψ2, has

lower energy

than Ψ1. Moreover, there is a jump in energy

between these states, hence the energy gap

band theory of solids17
Band Theory of Solids

The allowed ranges of the wave vector k are

called Brillouin zones.

zone 1: -p/a < k < p/a; zone 2: -2p/a < - p/a;

zone 3: p/a < k < 2p/a etc.

The theory can explain why some

substances are conductors, some

insulators and

others

semi

conductors

conductors insulators semiconductors
Conductors, Insulators, Semiconductors

Sodium (Na) has one electron in the 3s state, so

the 3s energy level is half-filled. Consequently, the

3s band, the valence band, of solid

sodium is also half-filled. Moreover,

the 3p band, which for Na is

the conduction band, overlaps with

the 3s band.

So valence electrons can easily be

raised to higher energy states.

Therefore, sodium is a good

conductor

conductors insulators semiconductors19
Conductors, Insulators, Semiconductors

NaCl is an insulator, with a band gap of 2 eV,

which is much larger than the thermal energy at

T=300K

Therefore, only a tiny fraction of electrons are

in the conduction band

conductors insulators semiconductors20
Conductors, Insulators, Semiconductors

Silicon and germanium have band gaps of 1 eV and

0.7 eV, respectively. At room temperature, a small

fraction of the electrons are in the conduction

band. Si and Ge are intrinsic semiconductors

summary
Summary
  • The heat capacity of the electron gas is small compared with that of the ions
  • Energy gaps arise in solids because they contain standing wave states
  • The size of the energy gap between the valence and conduction bands determines whether a substance is a conductor, an insulator or a semiconductor
ad