1

Solid State Electronics

Text Book

Ben. G. Streetman and Sanjay Banerjee: Solid State

Electronic Devices, Prentice-Hall of India Private

Limited.

Chapter 3

2

Bonding forces in SolidsBond: The interaction of electrons in neighboring atoms is called bond.

Ionic bond: Ionic bonds are a type of chemical bond based on electrostatic

forces between two oppositely-charged ions.

In ionic bond formation, a metal donates an electron, due to a low

electronegativity to form a positive ion.

The bonds between the sodium (Na) and chlorine (Cl) ions are ionic bonds.

The electronic structure of Na (Z=11) is [Ne]3s1, and Cl(Z=17) has the structure

[Ne]3s23p5.

Na atom gives up its outer 3s electron to a Cl atom, so that the crystal is made up

of ions with electronic structures of the inert atoms Ne and Ar.

However, the ions have net electric charges after the electron exchange.

The Na+ ion has a net positive charge, having lost an electron, and the Cl- ion has

a net negative charge, having gained an electron.

Once the electron exchanges have been made between the Na and Cl atoms to

form Na+ and Cl- ions, the outer orbits of all atoms are completely filled.

Since the ions have the closed-shell configurations of the inert atoms Ne and Ar,

there are no loosely bound electrons to participate in current flow; as a result,

NaCl is a good insulator.

3

Metallic bond: Metallic bonding is the bonding within metals. It

involves the delocalized sharing of free electrons among a lattice

(the periodic arrangement of atoms in a crystal is called the lattice)

of metal atoms.

In a metal atom the outer electron shell is only partially filled,

usually by no more than three electrons.

In Na has only one electron in the outer orbit.

This electron is loosely bound and is given up easily in ion

formation.

In the metal the outer electron of each alkali atom is contributed to

the crystal as a whole, so that the solid is made up of ions with

closed shells immersed in a sea of free electrons.

The forces holding the lattice together arise from an interaction

between the positive ion cores and the surrounding free electrons.

This is one type of metallic bonding.

The metals have the sea of electrons in common, and these

electrons are free to move about the crystal under the influence of

an electric field.

4

Covalent bond: Covalent bonding is an intermolecular form of

chemical bonding characterized by the sharing of one or more

pairs of electrons between two components, producing a mutual

attraction that holds the resultant molecule together.

Atoms tend to share electrons in such a way that their outer

electron shells are filled.

Atom in the Ge, Si, or C diamond lattice is surrounded by four

nearest neighbors, each with four electrons in the outer orbit.

In these crystals each atom shares its valence electrons with its

four neighbors.

The bonding forces arise from a quantum mechanical interaction

between the shared electrons.

This is known as covalent bonding; each electron pair constitutes a

covalent bond.

5

Energy Bands

The electron in an isolated atom has discrete energy level but

the electron in a solid has a range, or band, of available

energies.

The discrete energy levels of the isolated atom spread into

bands of energies in the solid because in the solid the wave

functions of electrons in neighboring atoms overlap, and an

electron is not necessarily localized at a particular atom.

As isolated atoms are brought together to form a solid,

various interactions occur between neighboring atoms.

The forces of attraction and repulsion between atoms will find

a balance at the proper interatomic spacing for the crystal.

In the process, important changes occur in the electron energy

level configuration and these changes result in the varied

electrical properties of solid.

6

Fig. (a) shows the curve of wave function

which is obtained from the solution of

Schrodinger Wave Equation.

(a)

Fig. (b) shows the orbital model of a Si

atom, which has a nucleus consisting of 14

protons (with a charge of +14) and neutrons,

10 core electrons in shells n=1 and 2, and 4

valance electrons in the 3s and 3p subshells.

Fig. (c) shows the energy levels of the

various electrons in the coulombic potential

well of the nucleus . Since unlike charges

attract each other, there is an attractive

potential between the negatively charged

electrons and the positively charged nucleus.

The Coulomb potential varies only with

radius in spherical coordinates

7

2 1

+ +

+

_

Atomic orbitals

Anti-bonding

orbital

Bonding orbital

Anti-bonding energy level

Bonding energy level

V(r)

Figure 3-2 Linear combination of atomic orbitals (LCAO): The

LCAO when 2 atoms are brought together leads to 2 distinct

“normal” models-a higher energy anti-bonding orbital, and a

lower energy bonding orbital.

In Fig. 3-2, the coulombic

potential wells of two atoms close

to each other, along with the

wave functions of two-electron

centered on the two nuclei are

schematically shown.

By solving the Schrodinger for

such an interacting system, it is

found that the composite two

electron wave functions are linear

combinations of the individual

atomic orbits (LCAO).

The odd or anti-symmetric

combination is called the anti-

bonding orbital, while the even or

symmetric combination is the

bonding orbital.

It is seen that the bonding orbital

has a higher value of the wave

function than the anti-bonding

state in the region between the

two nuclei.

8

2 1

Atomic orbitals

Anti-bonding energy level

Bonding energy level

V(r)

To determine the energy levels

of the bonding and anti-bonding

states, it is important to

recognize that in the region

between the two nuclei the

coulombic potential energy V(r)

is lowered (solid line in Fig. 3)

compared to isolated atoms

(dashed line in Fig. 3-2).

The potential energy in the

region is lowered because an

electron here would be attracted

by two nuclei; rather than just

one.

For the bonding state the electron probability density is higher in this region of

lowered potential energy than for the anti-bonding state.

As a result, the original isolated atomic energy level would be split into two, a lower

bonding energy level and a higher anti-bonding level.

9

We consider N atoms of silicon in a solid.

Each isolated silicon atom has an electron structure 1s22s22p63s23p2 in

the ground state.

There will be 2N, 2N, 6N, 2N, and 6N states of type 1s, 2s, 2p, 3s, and

3p, respectively.

As the interatomic spacing decreases, these energy levels split into

bands, beginning with the outer (n=3) shell.

As the “3s” and “3p” bands grow, they merge into a single band

composed of mixture of energy levels.

This band of “3s-3p” levels contains 8N available states.

As the distance between atoms approaches the equilibrium interatomic

spacing of silicon, this band splits into two bands separated by an energy

gap Eg.

The upper band (called the conduction band) contains 4N states, as does

the lower (valence) band.

10

The energy gap is sometimes

called a “forbidden band,”

since in a perfect crystal it

contains no electron states.

There are 4N electrons in the

original isolated n=3 shells (2N

in 3s states and 2N in 3p

states).

These 4N electrons must

occupy states in the valence

band or the conduction band in

the crystal.

At 0K the electrons will occupy the lowest energy states available to

them. In the case of Si crystal, there are exactly 4N states in the valence

band available to the 4N electrons. Thus at 0K, every state in the

valence band will be filled, while the conduction band will be

completely empty of the electrons.

11

Metals, Semiconductors, and Insulators

Insulator: A very poor conductor of electricity is

called an insulator.

In an insulator material the valance band

is filled while the conduction band is empty.

The conduction band and valance band in

the insulator are separated by a large forbidden

band or energy gap (almost 10 eV).

In an insulator material, the energy which

can be supplied to an electron from a applied field

is too small to carry the particle from the field

valance band into the empty conduction band.

Since the electron cannot acquire

sufficient applied energy, conduction is

impossible in an insulator.

12

Semiconductor: A substance whose conductivity lies between

insulator and conductor is a semiconductor.

A substance for which the width of the forbidden energy

region is relatively small (almost 1 eV) is called semiconductor.

In a semiconductor material, the energy which can be supplied to

an electron from a applied field is too small to carry the particle

from the field valance band into the empty conduction band at 0

K.

As the temperature is increased, some of the valance band

electrons acquire thermal energy. Thus, the semiconductors allow

for excitation of electrons from the valance band to conduction

band.

These are now free electrons in the sense that they can move

about under the influence of even a small-applied field.

Metal: A metal is an excellent conductor.

In metals the band either overlap or are only partially

filled.

Thus electrons and empty energy states are intermixed within the

bands so that electrons can move freely under the influence of an

electric field.

13

Direct and Indirect SemiconductorsA single electron is assumed to travel through a perfectly periodic

lattice.

The wave function of the electron is assumed to be in the form of a

plane wave moving.

For example, in the x-direction with propagation constant k, also called

wave vector.

The space-dependent wave function for the electron is

where the function U(kx,x) modulates the wave function according to

the periodicity of the lattice.

Depending on the transition of an electron from conduction band to

valance band with respect to the propagation constant, the

semiconductor materials are classified as follows:

(a) Direct semiconductor and

(b) Indirect semiconductor

)13(),()( xxj

exxUxk

kk

14

Direct Material: The material (such as

GaAs) in which a transition of an electron

from the minimum point of conduction band

to the maximum point of valence band takes

place with the same value of K (propagation

constant or wave vector) is called direct

semiconductor material.

According to Eq. (3-1) the energy (E) vs

propagation constant (k) curve is shown in

the figure.

A direct semiconductor such as GaAs, an

electron in the conduction band can fall to an

empty state in the valence band, giving off

the energy difference Eg as a photon of light.

15

Indirect Material: The material (such as Si) in

which a transition of an electron from the

minimum point of conduction band to the

maximum point of valence band takes place

with the different values of K (propagation

constant or wave vector) is called indirect

material.

According to Eq. (3-1) the energy (E) vs

propagation constant (k) curve is shown in the

figure.

An electron in the conduction band minimum of an indirect

semiconductor cannot fall directly to the valence band maximum but

must undergo a momentum change as well as changing its energy.

It may go through some defect state (Et) within the band gap.

In an indirect transition which involves a change in k, the energy is

generally given up as heat to the lattice rather than as emitted photon.

16

Electrons and Holes

Hole: An empty state in the valence band is referred to as a

hole.

Electron-Hole Pair: If the conduction band electron and

the hole are created by the excitation of the valence band

electron to the conduction band, they are called an

electron-hole pair (abbreviated EHP).

17

If a filled band, all available energy states are occupied.

For every electron moving with given velocity, there is an equal and

opposite electron motion elsewhere in the band.

If we apply an electric field, the net current is zero because for every

electron j moving velocity vj there is a corresponding electron j‟ with

the velocity –vj.

Fig. 3-8 illustrates this effect in terms of the electron vs. wave vector

plot for the valance band.

Since k is proportional to electron momentum, it is clear the two

electrons have opposite directed velocities.

Fig. 3-8

With N electron/cm3 in the band we express

the current density using a sum over all of

the electron velocities, and including the

charge –q on each electron.

In a unit volume,

)23()bandfilled(0)( aN

iivqJ

18

Now if we create a hole by removing the jth electron, the net current

density in the valance band involves the sum over all velocities, minus

the contribution of the electron we have removed.

)23()missingelectronth(0)()( bjN

ijvqivqJ

Since the first term of (3-2b) is zero in accordance (3-2a), the net

current is

)electronjthofmissingthetoduecurrentNet(jqvJ

The current contribution of the hole is equivalent to that of a positively

charged particle with the velocity vj that of the missing electron.

The charge transport is actually due to the motion of the new

uncompensated electron j’. Its current contribution (-q)(-vj) is

equivalent to that of a positively charged particle with the velocity vj.

Thus, it is realized that the current flow in the semiconductor can be

account by the motion of electrons and holes of charge carriers.

19

In the valence band, hole energy increases oppositely to electron

energy, because the two carriers have opposite charge.

Thus hole energy increases downward in Fig. 3-8 and holes, seeking

the lowest energy state available, are generally found at the top of the

valance band.

In contrast, conduction band electrons are found at the bottom of the

conduction band.

Holes are found at the top of the valence band

because the valence band electrons will

rearrange themselves so that they occupy the

lowest energy states, leaving only the highest

energy level vacant in the valance band.

Electrons in the conduction band will

similarly rearrange themselves so they

occupy the lowest energy states of

conduction band. Fig. 3-8

20

Effective Mass

The electrons in a crystal are not completely free, but instead

interact with periodic potential of the lattice of a crystal.

The electron “wave particle” motion cannot be expected to be

the same as for electrons in free space.

And, the mass of free electron is not same as for electrons in

a solid.

The electron momentum can be written as P=mv=ħk. Then

22

22212

21 k

mmPmvE

Thus the electron energy is parabolic with wave vector k.

21

The electron mass is inversely related to the curvature

(second derivative) of the (E, k) relation, since

mdEd 22

2 k

The effective mass of an electron in a band with a given (E,

k) relationship is found as follows:

2/22*

kdEdm

Thus, the mass of electron which is obtained from the

curvature of the energy band of a solid is called effective

mass.

22

Intrinsic MaterialA perfect semiconductor with no impurities or lattice defect is

called an intrinsic material.

In intrinsic material, there are no charge carrier at 0K, since the

valence band is filled with electrons and the conduction band is

empty.

At high temperature electron-hole pairs are generated as valence

band electrons are excited thermally across the band gap to the

conduction band.

These EHPs are the only charge carriers in intrinsic material.

Since the electrons and holes are crated in pairs, the conduction

band electron concentration n (electron/cm3) is equal to the

concentration of holes in the valence band p (holes/cm3).

Each of these intrinsic carrier concentrations is commonly

referred to as ni. Thus for intrinsic material: n=p=ni (3-6)

At a temperature there is a carrier concentration of EHPs ni.

23

Recombination is occurs when an electron in the conduction

band makes transition to an empty state (hole) in the valence

band, thus annihilating the pair.

If we denote the generation rate of EHPs as gi (EHP/cm3-s)

and the recombination rate ri, equilibrium requires that

ri=gi (3-7a)

Each of these rates is temperature dependent.

gi(T) increases when the temperature is raised, and a new

carrier concentration ni is established such that the higher

recombination rate ri(T) just balances generation.

At any temperature, the rate of recombination of electrons

and holes ri is proportional to the equilibrium concentration

of electrons n0 and the concentration of holes p0:

ri=arn0p0= arni2=gi (3-7b)

The factor ar is a constant of proportionality which depends

on the particular mechanism takes place.

24

Extrinsic Material

When a crystal is doped such that the equilibrium carrier

concentrations n0 and p0 are different from carrier concentration

ni, the material is said to be extrinsic material.

In addition to the intrinsic carriers generated, it is possible to

create carriers in semiconductors by purposely introducing

impurities into the crystal.

This process, called doping, is the most common technique for

varying conductivity of semiconductor.

There are two types of doped semiconductors, n-type (mostly

electrons) and p-type (mostly holes).

An impurity from column V of the periodic table (P, As and Sb)

introduces an energy level very near the conduction band in Ge or

Si.

25

The energy level very near the conduction band is filled with electrons

at 0K, and very little thermal energy is required to excite these

electrons to the conduction band (Fig. 3-12a).

Thus at 50-100K virtually all of the electrons in the impurity level are,

“donated” to the conduction band.

Such an impurity level is called a donor level and the column V

impurities in Ge or Si are called donor impurities.

Semiconductors doped with a significant number of donor atoms will

have n0>>(ni,p0) at room temperature.

Fig. 3-12 (a) Donation of

electrons from donor level to

conduction band.

This is n-type material.

26

Similarly, an impurity from column III of the periodic table (B, Al, Ga

and In) introduces an energy level very near the valence band in Ge or

Si.

These levels are empty of electrons at 0K (Fig. 3-12b).

At low temperatures, enough thermal energy is available to excite

electrons from the valence into the impurity level, leaving behind holes

in the valence band.

Since this type of impurity level “accepts” electrons from the valence

band, it is called an acceptor level, and the column III impurities are

acceptor impurities in the Ge and Si.

Fig. 3.12b

Doping with acceptor

impurities can create a

semiconductor with a hole

concentration p0 much greater

that the conduction band

electron concentration n0.

This type is p-type material.

27

Carrier concentrationThe calculating semiconductor properties and analyzing device

behavior, it is often necessary to know the number of charge carriers

per cm3 in the material.

To obtain equation for the carrier concentration, Fermi-Dirac

distribution function can be used.

The distribution of electrons over a range of allowed energy levels at

thermal equilibrium is

kTFEEe

Ef/)(

1

1)(

where, k is Boltzmann’s constant (k=8.2610-5 eV/K=1.3810-23

J/K).

The function f(E), the Fermi-Dirac distribution function, gives the

probability that an available energy state at E will be occupied by an

electron at absolute temperature T.

The quantity EF is called the Fermi level, and it represents an

important quantity in the analysis of semiconductor behavior.

28

For an energy E equal to the Fermi level energy EF, the occupation

probability is

2

1

1

1)(

/)(

kTFEFEFe

Ef

The significant of Fermi Level is that the probability of electron and

hole is 50 percent at the Fermi energy level. And, the Fermi function

is symmetrical about EF for all temperature; that is, the probability

f(EF +E) of electron that a state E above EF is filled is the same as

probability [1-f(EF-E)] of hole that a state E below EF is empty.

At 0K the distribution takes the

simple rectangular form shown in

Fig. 3-14.

With T=0K in the denominator of

the exponent, f(E) is 1/(1+0)=1

when the exponent is negative

(E<EF), and is 1/(1+)=0 when

the exponent is positive (E>EF).

29

This rectangular distribution implies that at 0K every available energy

state up to EF is filled with electrons, and all states above EF are empty.

At temperature higher than 0K, some probability exists for states above

the Fermi level to be filled.

At T=T1 in Fig. 3-14 there is

some probability f(E) that states

above EF are filled, and there is

a corresponding probability [1-

f(E)] that states below EF are

empty.

The symmetry of the

distribution of empty and filled

states about EF makes the Fermi

level a natural reference point

in calculations of electron and

hole concentration in

semiconductors.

30

Fig. 3-15(a) Intrinsic Material

For intrinsic material, the concentration of holes in

the valence band is equal to the concentration of

electrons in the conduction band.

Therefore, the Fermi level EF must lies at the middle

of the band gap.

Since f(E) is symmetrical

about EF, the electron

probability „tail‟ if f(E)

extending into the conduction

band of Fig. 3-15a is

symmetrical with the hole

probability tail [1-f(E)] in the

valence band.

31

In n-type material the Fermi level lies near

the conduction band (Fig. 3-15b) such that

the value of f(E) for each energy level in the

conduction band increases as EF moves

closer to Ec.

Thus the energy difference (Ec- EF) gives

measure of n.

Fig. 3.15(b) n-

type material

Fig. 3.15(c) p-

type material

In p-type material the Fermi level lies

near the valence band (Fig. 3-15c) such

that the [1- f(E)] tail value Ev is larger

than the f(E) tail above Ec.

The value of (EF-Ev) indicates how

strongly p-type the material is.

32

Example: The Fermi level in a Si sample at equilibrium is located at

0.2 eV below the conduction band. At T=320K, determine the

probability of occupancy of the acceptor states if the acceptor states

relocated at 0.03 eV above the valence band.

Solution:

From above figure, Ea-EF={0.03-(1.1-0.2)} eV= -0.87 eV

kT= 8.6210-5 eV/K320=2758.4 eV

we know that,

0.1

1

1

1

1)(

)5104.2758/(87.0/)(

eeEf

kTFEaEa

33

Electron and Hole Concentrations at Equilibrium

The concentration of electron and hole in the conduction band and

valance are

where N(E)dE is the density of states (cm-3) in the energy range dE.

The subscript 0 used with the electron and hole concentration symbols

(n0, p0) indicates equilibrium conditions.

The number of electrons (holes) per unit volume in the energy range

dE is the product of the density of states and the probability of

occupancy f(E) [1-f(E)].

Thus the total electron (hole) concentration is the integral over the

entire conduction (valance) band as in Eq. (3.12).

The function N(E) is proportional to E(1/2), so the density of states in

the conduction (valance) band increases (decreases) with electron

(hole) energy.

)12.3()()](1[

)12.3()()(

0

0

bdEENEfp

adEENEfn

vE

cE

34

Similarly, the probability of finding an empty state (hole) in the

valence band [1-f(E)] decreases rapidly below Ev, and most hole

occupy states near the top of the valence band.

This effect is demonstrated for intrinsic, n-type and p-type materials

in Fig. 3-16.

Fig. 3.16 (a) Concentration of electrons and holes in intrinsic material.

35

Fig. 3.16 (b) Concentration of electrons and holes in n-type material.

Fig. 3.16 (a) Concentration of electrons and holes in p-type material.

36

The electron concentration (in terms of effective density of states Nc

which is located at the conduction band edge Ec) in thermal

equilibrium can also be written as follows:

)13.3()(0 cc EfNn 2/3

2

*22where,

h

kTmN n

c

It is assumed that the Fermi level EF lies at least several kT below the

conduction band.

Then and the Fermi function f(Ec) can be simplified

as1

/)(

kTFEcEe

)14.3(1

1)(

/)(

/)(

kTFEcE

kTFEcEc ee

Ef

For this condition the concentration of electrons in the conduction

band is

)15.3(/)(

0kTFEcE

ceNn

37

By similar argument, the hole concentration (in terms of effective

density of states Nv which is located at the valance band edge Ev) in

thermal equilibrium can also be written as follows:

)16.3()](1[0 vv EfNp 2/3

2

*22where,

h

kTmN

pv

For EF larger than Ev by several kT, the probability of finding an

empty state at Ev is

)17.3(1

11)(1

/)(

/)(

kTvEFE

kTFEvEv ee

Ef

For this condition the concentration of holes in the valance band is

)18.3(/)(

0kTvEFE

veNp

38

The electron and hole concentrations predicted by Eqs. (3-15) and (3-

18) are valid whether the material is intrinsic or doped, provided

thermal equilibrium is maintained.

Thus for intrinsic material, EF lies at some intrinsic level Ei near the

middle of the band gap, and the intrinsic electron and hole

concentrations are

)21.3(,/)(/)( kTvEiE

vikTiEcE

ci eNpeNn

From Eqs. (3.15) and (3.18), we obtain

kTvEFEv

kTFEcEc eNeNpn

/)(/)(00

)22.3(//)(

00

kTgE

vckTvEcE

vc eNNeNNpn

39

From Eq. (21), we obtain

)23.3(//)( kTgE

vckTvEcE

vcii eNNeNNpn

kTvEiEv

kTiEcEcii eNeNpn

/)(/)(

From Eqs. (3.22) and (3.23), the product of n0 and p0 at equilibrium is

a constant for a particular material and temperature, even if the

doping is varied.

The intrinsic electron and hole concentrations are equal, ni=pi; thus

from Eq. (3.23) the intrinsic concentrations is

)24.3(2/ kTgE

vci eNNn

The constant product of electron and hole concentrations in Eq. (3.24)

can be written conveniently from (3.22) and (3.23) as

)25.3(200 inpn

At room temperature (300K) is: For Si approximately ni=1.51010

cm-3; For Ge approximately ni=2.51013 cm-3;

40

)26.3(/)(

/)(

kTvEiEiv

kTiEcEic

epN

enN

From Eq. (3.21), we can write as

kTFEcEiEcEi

kTFEcEkTiEcEi eneenn

/)(/)(/)(0

Substitute the value of Nc from (3.26) into (3.15), we obtain

)27.3(/)(/)(

0kTiEFE

ikTFEiE

i enenn

Substitute the value of Nv from (3.26) into (3.18), we obtain

kTvEFEvEiEi

kTvEFEkTvEiEi eneepp

/)(/)(/)(0

)28.3(/)(/)(

0kTFEiE

ikTiEFE

i enenp

It seen from the equation (3.27) that the electron concentrations n0

increases exponentially as the Fermi level moves away from Ei

toward the conduction band.

Similarly, the hole concentrations p0 varies from ni to larger values as

EF moves from Ei toward the valence band.

41

Example 3-5 A Si sample is doped with 1017 As atoms/cm3. What is the

equilibrium hole concentration p0 at 300K? Where is EF relative to Ei?

Solution: Nd=1017atoms/cm3; kT=0.0259eV; ni(for Si)=1.51010 cm-3;

Since Nd>>ni, we can approximate n0=Nd

33

17

210

0

2

0 cm1025.210

)105.1(

n

np i

We know that kTiEFEienn

/)(0

eV407.0

105.1

10ln0259.0

ln

10

17

0

iF

iF

iiF

EE

EE

n

nkTEE

The resulting band diagram

is

42

Temperature Dependence of Carrier

Concentrations

The variation of carrier concentration with temperature is indicated

by Eq. (3.21)

The intrinsic carrier ni has a strong temperature dependence (Eq.

3.24) and that EF can vary with temperature.

)21.3(,/)(/)( kTvEiE

vikTiEcE

ci eNpeNn

)24.3(2/ kTgE

vci eNNn

The temperature dependence of electron concentration in a doped

semiconductor can be visualized as shown in Fig. 3-18.

43

Figure 3-18 Carrier concentration vs.

inverse temperature for Si doped with

1015 donors/cm3.

In this example, Si is doped

n-type with donor

concentration Nd of 1015 cm-3.

At very low temperature

(large 1/T) negligible intrinsic

EHPs exist, and the donor

electrons are bound to the

donor atoms.

As the temperature is raised,

these electrons are donated to

the conduction band, and at

about 100K (1000/T=10) all

the donor atoms are ionized.

This temperature range is

called ionization region.Once the donor atoms are ionized, the conduction band electron

concentration is n0Nd=1015 cm-3, since one electron is obtained for each

donor atom.

44

When every available extrinsic electron has been transferred to the

conduction band, no is virtually constant with temperature until the

concentration of intrinsic carriers ni becomes comparable to the

extrinsic concentration Nd.

Finally, at higher temperature ni is much greater than Nd, and the

intrinsic carriers dominate.

In most devices it is desirable to

control the carrier concentration by

doping rather than by thermal EHP

generation.

Thus one usually dopes the material

such that the extrinsic range extends

beyond the highest temperature at

which the device to be used.

45

Compensation and Space Charge Neutrality

Figure 3.19 Compensation

in an n-type semiconductor

(Nd>Na)

If a semiconductor contains both donors and acceptors.

For example, Fig. 3.19 illustrates a semiconductor for which both

donor and acceptors are present, but Nd>Na.

The predominance of donors makes the material n-type, and the

Fermi level is therefore in the upper part of the band gap.

Since EF is well above acceptor level

Ea, this level is essentially filled with

electrons. However, With EF above Ei,

it cannot be expected that a hole

concentration in valence band

commensurate with the acceptor

concentration.

In fact, the filling of the Ea states occurs

at the expense of the donated

conduction band electrons.

46

This mechanism can be visualized as follows:

Assume an acceptor state is filled with a valence band electrons

with a hole resulting in the valence band.

This hole is then filled by recombination with one of the conduction

band electrons.

Extending this logic to all the acceptor atoms, it is expected that the

resultant concentration of electrons in the conduction band to be Nd-

Na instead of the total Nd.

This process is called compensation.

By this process it is possible to begin with an n-type semiconductor

and add acceptors until Na=Nd and no donated electrons remain in

the conduction band.

In such compensated material n0=ni=po, and intrinsic conduction is

obtained.

With further acceptor doping the semiconductor becomes p-type

with a hole concentration of essentially Na-Nd.

47

The exact relationship among the electron, hole, donor and acceptor

concentrations can be obtained by considering the requirements for

space charge neutrality.

If the material is to remain electrostatically neutral, the sum of the

positive charges (holes and ionized donor atoms) must balance the

sum of the negative charges (electrons and ionized acceptor atoms):

)27.3(00 ad NnNp

Thus in Fig 3.19 the net electron concentration in the conduction

band is )28.3()(00 ad NNpn

If the material doped n-type (n0>>p0) and

all the impurities are ionized, we can

approximate Eq. (3-28) by

ad NNn 0

48

Example: A Si is doped with 91015 cm-3 donors and 31015

acceptors. Find the position of the Fermi level at 40C.

Solution: Nd=91015 cm-3; Na=31015 cm-3; ni=1.51010 cm-3;

Since Nd>Na, the Fermi level near to the donor states.

We obtain, Nrd=Nd-Na=61015 cm-3 donor atoms; Thus the Fermi

level depends on the donor atoms Nrd.

Now we consider n0=Nrd because Nrd>>ni. T=(273+40)K=313K

So we obtain, iiF nnkTEE /ln 0

)105.1/()106(ln)313)(/1062.8( 10155 KKeVEE iF

348.0 iF EE

The resulting band diagram is

49

End of

Chapter 3