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SEMICONDUCTOR DEVICES & TECHNOLOGY EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

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Page 1: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

SEMICONDUCTOR DEVICES &

TECHNOLOGY

EE4209

Instructor:Md. Nur Kutubul AlamDepartment of EEEKUET

Page 2: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Analogy of water and current flow

Water flows at non-equilibrium condition only.

Page 3: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Equilibrium situation

Arbitrary reference level

mghw

mghg

Potential energy, mghw < mghg

That is why water can not reach to river bank. And at the same time, water has a maximum height or level above which there is no water. This level is called Fermi level

Fermi level

hw < hg

Page 4: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Small disturbance to the Equilibrium

Arbitrary reference level

mghw

mghg

Fermi level

Small disturbance like wind or storm can create a wave of water. In this condition, a very small fraction of total river water can go above the fermi level.

Page 5: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Movement of water

Arbitrary reference level

mghw

mghg

Fermi level 1Fermi level 2

If we dig a pond in the river bank, it will be at a larger height than river water. But the pond water also has a fermi level and this level is at a higher position than that of river water until they are disconnected from each other.

Page 6: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Movement of water

Arbitrary reference level

mghw

mghg

Fermi level 1Fermi level 2

Now, if we remove the barrier between pond water and river water, water will flow from pond to river.WHY????

• Pond water had a higher potential energy and physical body wants to minimize its energy.

• In another sense, pond water had higher fermi level and no two system wants different fermi level, when they are connected by appropriate mean. They want a single fermi level which implies the equilibrium.

Page 7: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Its all about Energy

Arbitrary reference level

mghw

mghg

Fermi level

To be at any geometric position of the land, water needs a minimum amount of energy depending upon that position. For example, at a position where the pond was dug (see few slide back), water needs “mghg” amount of energy to be there.

Page 8: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Its all about Energy

Arbitrary reference level

mghw

mghg

Fermi level

To be at any geometric position of the land, water needs a minimum amount of energy depending upon that position. For example, at a position where the pond was dug (see few slide back), water needs “mghg” amount of energy to be there.

And the maximum amount of energy that water has is equal to the “fermi level”

Page 9: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Its all about Energy

Arbitrary reference level

Fermi level

And the maximum amount of energy that water has is equal to the “fermi level”

Page 10: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Energy profile/diagram

Arbitrary reference level

Fermi level

Energy

Position, x

Graph of required energy to be somewhere, at position ‘x’

Maximum available energy is the “fermi energy”

So, positions where required energy<fermi level, are covered with water

Page 11: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Energy profile/diagram

Fermi level

Energy

Position, x

Every concept we discussed so far on water, is similar for electron inside a solid.

Previously, this was a graph of “required energy” of water on earth. Now consider it is the graph of “required energy” of electron inside a solid.Water always flow downward in energy diagram and so the electron.

Page 12: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Energy profile/diagram

Fermi level

Energy

Position, x

So, just like water,if you put an electron to the left, it will travel to the right side and will be somewhere where the “required energy” is bellow the fermi level.

And what does it physically mean?

Page 13: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Physical meaning of Energy profile

Fermi level

Energy

Position, x

Position, x

Consider a semiconductor bar shown above and let, the diagram bellow is the “Required potential energy” inside it. Now let, a photon strikes to the left of the bar and created an electron.

Page 14: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Physical meaning of Energy profile

Fermi level

Energy

Position, x

Position, x

Page 15: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Water vs Electron (Energy view point)

As said previously, Everything we discussed previously for water, is applicable for electron also!

You can say river of electron instead of river of water. So-• Concept of position dependant energy (or

required energy) be the same• Maximum energy of electron (at absolute zero

temperature) is equal to the fermi level.• At non-zero temperature, i,e when electron sea

is not calm, some electrons will have energy higher than fermi level.

Page 16: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Brief about potential energy, or “the band diagram”

• Electron will go to minimum energy position• This potential energy diagram is also known as “band diagram”.

Page 17: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

How to find this potential diagram or band diagram?

Answer: Calculate the potential energy some how!

Example:Take a semiconductor bar and put a voltage ‘VG’ as shown. Assume resistance of the bar be R.

At x=0, Potential=VG volt

At x=L, Potential=0 voltBut what in between?

To understand easily, assume the total resistance R is composed of many series connected resistance ‘r’ as shown.

Now, from right side (x=L),Voltage after 1st resistor, V1=0+irVoltage after 2nd resistor, V2=V1+irVoltage after 3rd resistor, V3=V2+ir and so on

x

L

voltageVG

V1V2V3

VG

Page 18: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

How to find this potential diagram or band diagram?

x

voltageVG

LExact Mathematical technique to get this potential profile is to solve the poisson’s equation,

For a simpler case here, let n(x)=0. That means there is no charge in the semiconductor bar. (It is true only for intrinsic semiconductor or for insulator)Then,

At x=0, V=VG

At x=L, V=0

C2 = VG

C1 = - C2/L So V=VG - (VG/L).x

VG

Page 19: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

How to find this potential diagram or band diagram?

x

voltage

L

V1V2V3

Now we have the potential (voltage) distribution along the semiconductor bar.

And we know, energy required +1C charge at a position is called potential of that point ‘V’. Hence energy required to bring q coluomb chare, E=qV

So energy required to bring one electron, E= -eV

Energy of electron

-eV

x

VG

VG

Page 20: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

The band diagram

x

voltage

L

-eV

Strange!At x=0, energy of electron = -eV

How energy can be negative???

Actually absolute energy in the system of semiconductor bar is not negative. It means, upon application of voltage, energy of electron at x=0 is reduced by the amount “eV” with respect to the energy at x=L

x

Energy of electron

VG

VG

Page 21: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Significance of Band diagram

x

voltage

L

-eV

So what will happen then?

If there was an electron at x=L, after application of voltage, electron will see that it will have less amount of energy at x=0.So, it will travel towards the left to have minimum amount of energy.

The result is obvious because,The positive voltage of the battery will attract the electron from x=L (rightmost) to x=0 (left most) position. x

Energy of electron

VG

VG

Page 22: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Operation of FETUpon application of positive voltage at the gate (+Vg), electrons come close to gate terminal. The more positive Vg, the more electron near gate region and vice versa.

Then drain current,Id = - nAvyevy =μEy

Id = - nAe μEy

Id = - nAe μ(dVd /dy)

If Vd is fixed, thenId α Vg

[N.B: This is true only in linear region]

Drain

Source

VG

Page 23: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

FET operationOne very important question.

When we put a positive voltage in the gate, why electron does not come to the gate metal from the semiconductor and produce a current in gate circuit???

Or why does the gate voltage only cause the movement of electron inside the semiconductor only???

Page 24: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

FET operationOne very important question.

When we put a positive voltage in the gate, why electron does not come to the gate metal from the semiconductor and produce a current in gate circuit???

Or why does the gate voltage only cause the movement of electron inside the semiconductor only???

Page 25: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

FET operationOne very important question.

When we put a positive voltage in the gate, why electron does not come to the gate metal from the semiconductor and produce a current in gate circuit???

Or why does the gate voltage only cause the movement of electron inside the semiconductor only???

All physical connections are established here. So the circuit is complete. Then should not the electron flow like this??????

Why does not it do so?

Page 26: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

FET operationAnswer is for the energy barrier.

At x=0, there is a change in energy from lower value to a higher value which was not told previously. It is just like an energy hill, called a “barrier”. This energy hill or barrier opposes the electron to come into the metal from the semiconductor.

X=0 X=LX= -a

Energy

Electron can not overcome this energy barrier and hence can not come into the metal conductor.

Now the question is, how to create this energy barrier?

VG

Page 27: EE4209 Instructor: Md. Nur Kutubul Alam Department of EEE KUET

Creation of energy barrier

Answer is simple! By making a junction of two different materials.

So, possible options are-• Metal-semiconductor schottky

junction• Metal-insulator-semiconductor

structure• Semiconductor-semiconductor

heterojunction

X=0 X=LX= -a

Energy

To understand each of these thing clearly, we will pay our attention to the junction (or interface of semiconductor and external gate circuit).

VG