energy bands and gaps in semiconductor

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A SEMINAR ON ENERGY BANDS AND GAPS IN SEMICONDUCTOR K. GANAPATHI RAO (13031D6603) Presented By Presence of Mr. M. Venkaiah

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Energy bands and gaps in semiconductor

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Page 1: Energy bands and gaps in semiconductor

A SEMINAR ONENERGY BANDS AND GAPS

IN SEMICONDUCTOR

K. GANAPATHI RAO(13031D6603)

PresentedBy

Presence ofMr. M. Venkaiah

Page 2: Energy bands and gaps in semiconductor

Introduction Energy band Classification of materials Direct and indirect band gap of SC Classification of SC References

Out Line

Page 3: Energy bands and gaps in semiconductor

INTRODUCTION

Si= 14 electrons 1s2 2s2 2p6 3s2 3p2 4 valence electrons Electrons present in the outermost orbit are called valence

e- and their behavior decide electrical characteristics of a materials.

For Si 2 e- are present in 3s and 2 e- are in 3p orbital's Consider n Si atoms, which are for apart from each other so

that the interaction b/w them is negligible. In this 2N e- occupy the 3s level and 2N e- in 3p level. When the atoms are brought to closer, the interaction b/w

increases and they now form a electronic system.

Page 4: Energy bands and gaps in semiconductor

The electronic system should obey Paulie’s exclusion principal , which states that no 2 e- are in the system can have same amount of energy.

To obey this 3s and 3p level spilt into multiple levels so that each e- can occupy a district energy level.

When inter atomic distance is further reduced. The 2N ‘s’ levels and 6N ‘p’ levels combined into a single band.

At lattice spacing, single band is split into 2 bands with upper band containing 4N and lower band with 4N levels.

At 00 k e- possess lowest energy , they fill up valence band and conduction band remaining empty.

Page 5: Energy bands and gaps in semiconductor

There Important energy bands are,

Valence Band

Conduction Band

Forbidden Band

 

Energy Bands theory

Page 6: Energy bands and gaps in semiconductor

Valence Band

Band of energy level which are closer to nucleolus.

An e- in valence band, expenses strong force of attraction from nucleolus.

And it can’t move freely when extrenal electric field is applied.

It is called bounded electron.

Page 7: Energy bands and gaps in semiconductor

Conduction Band

Bond of energy levels which are far away from the nucleolus.

The conduction band is the band of orbitals that are high in energy and are generally empty.

 An e- in Conduction band has weak influence of nucleolus and hence it can move free under the effect of applied electric field and thus it produces current, it is called free electrons

Page 8: Energy bands and gaps in semiconductor

Forbidden Band / Energy Gap

In solid-state physics, an energy gap or bandgap, is an energy range in a solid where no electron states can exist.

It generally refers to the energy difference (in electron volts) between the top of the valence band and the bottom of the conduction band in insulators and semiconductors.

Page 9: Energy bands and gaps in semiconductor

Types of Materials

Materials can be divided into 3 types based on the values of energy gap

Insulator Conductor Semi Conductor

Page 10: Energy bands and gaps in semiconductor
Page 11: Energy bands and gaps in semiconductor

INSULATORS

It is a material with large energy gap Eg= several ev ev= 1.6*10-19 joules

Due to large energy gap an e- from valence band can’t move into conduction band remains complete fill.

Conduction band completly empty. Ex: glass, Diamond, Silicon di oxide

Energy gap of diamond is ~6ev.

Page 12: Energy bands and gaps in semiconductor

CONDUCTORS

It is a material having zero energy gap. The materials in which conduction and valence bands.

Valence electrons can move valence to conduction band without requiring thermal energy.

The overlapping indicates a large number of electrons available for conduction.

Hence the application of a small amount of voltage results a large amount of current.

Ex: All metals. Best conducting materials are

Silver is best, cupper is second best

Page 13: Energy bands and gaps in semiconductor

SEMICONDCUTOR

The materials, in which the conduction and valence bands are separeated by a small energy gap (1eV) are called semiconductors.

Silicon and germanium are the commonly used semiconductors.

A small energy gap means that a small amount of energy is required to free the electrons by moving them from the valence band in to the conduction band.

The semiconductors behave like insulators at 0K, because no electrons are available in the conduction band.

If the temperature is further increased, more valence elctrons will acquire energy to jump into the conduction band.

Page 14: Energy bands and gaps in semiconductor

If a valence receives sufficient thermal energy, it can move into conduction band leaving a vacancy in valence band, which is called hole and therefore, if one e- is sufficiently thermally energized it creates a pair of free e- and hole, this process is called carrier generation

Carrier generation can happen due to Thermal excitation Photo excitation Electrical excitation Impact ionization

Page 15: Energy bands and gaps in semiconductor

Eg (T)= 1.21-3.6*10-4 T for siEg (T)= 0.785-2.23*10-4 T for Ge

When external electric field is applied free electron travels with in conduction band producing electron current.

Where as hole travels in valence, producing hole current.

The total current will be sum of free & hole current. I total = I free e- + I hole

As temp increase free e- & holes will increase and conductivity increases.

Page 16: Energy bands and gaps in semiconductor

Direct & Indirect band gap SC

The process of free e- returning from conduction band to valence band which causes disappearance of a free e- , hole pair is called carrier recombination.

SC are divided into 2 types based upon the method of recombination. Direct band gap SC Indirect band gap SC

Page 17: Energy bands and gaps in semiconductor

Direct band gap SC

For these SC , Conduction band minima and valence band maxima occurs at same value of momentum.

An e- from CB directly return to VB without changing It’s momentum. And releases energy in the form of light (photon hv).

Ex: GaAS, Gap.GaAsP,

Page 18: Energy bands and gaps in semiconductor

Indirect band gap SC

CB minima and VB maxima occurs at different value of momentum.

When e- from CB returns VB after changing its momentum is called indirect band gap sc.

E- changes its momentum by releasing phonon which is a heat particle.

Ex: Si, Ge

Page 19: Energy bands and gaps in semiconductor

Intrinsic SC

IV group is carbon, Si, Ge, Tin, Lead. In it sc crystal each atom forms four covalent bonds to

become stable. At 00 , all valence e- participate in covalent band formation.

Conduction not possible. if temp is increases, greater no of free e- hole pair will be

created. Causes conduction n=p=ni

J=ni(un+up)eE

Page 20: Energy bands and gaps in semiconductor

N type SC

Vth group Phospurs, Arsenic, Antimon. P forms 4 covalent bonds with Si and donate 5th electron to

crystal. It is called free e-. According to law of Nutrality nn=pn+nD

Mass action law nn*pn=ni2

Majority is e-minority is holes

Page 21: Energy bands and gaps in semiconductor

P type SC

3rd group B, Al, Ga. B forms 3 covalent bonds with Si and forms 4th bond with

hole formation. According to law of Nutrality np +nA=pp

Mass action law np*pp=ni2

Majority is holesminority is e-

Page 22: Energy bands and gaps in semiconductor

References

http://en.wikipedia.org/wiki/Electronic_band_structure

http://ecee.colorado.edu/~bart/book/book/chapter2/ch2_3.htm

http://pubs.acs.org/doi/abs/10.1021/jz402165b http://iopscience.iop.org/0305-4608/5/11/020

Page 23: Energy bands and gaps in semiconductor