LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar...

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LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology Sathyamangalam

Transcript of LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar...

Page 1: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

LASERS

Dr D. Arun Kumar

Assistant Professor

Department of Physical Sciences

Bannari Amman Institute of Technology Sathyamangalam

Page 2: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

General Objective

• To understand the principle,

characteristics and types of LASER

Page 3: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Specific Objectives

1.state the principle of LASER (S)

2. list the four characteristics of LASER (S)

3.classify the five types of LASER with

examples (T)

4.analyse the two conditions to achieve

laser action (S)

Page 4: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Introduction

• LASER stands for Light amplification by

stimulated emission of radiation.

• Laser is a device which emits a powerful,

monochromatic collimated beam of light.

The emitted light waves are coherent in

nature.

Page 5: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Characteristics of Laser:

• Directionality – less divergence

• Intensity – one direction

• Monochromatic – single wave length

• Coherence - inphase

Page 6: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Principle of Spontaneous and Stimulated emission

• We know that, when light is absorbed

by the atoms or molecules, then it goes

from the lower energy level (E1) to the

higher energy level (E2)

• during the transition from higher energy

level (E2) to lower energy level (E1) the

light is emitted from the atoms or

molecules.

Page 7: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Let us consider an atom exposed to light

photons of energy , three distinct processes

take place.

a. Absorption

b. Spontaneous emission

c. Stimulated Emission

Principle of Spontaneous and Stimulated emission

Page 8: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Absorption• An atom in the lower energy level or

ground state energy level E1 absorbs the

incident photon radiation of energy hν and

goes to the higher energy level or excited

level E2

Page 9: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Spontaneous emission

• The atom in the excited state returns to

the ground state by emitting a photon of

energy E = (E2 – E1) = hν

Page 10: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Stimulated Emission

• external triggering or inducement of

photon thereby emitting a photon of

energy equal to the energy of the incident

photon

Page 11: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Differences between Stimulated

and spontaneous emission of

radiation

Page 12: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Population Inversion

• Population Inversion creates a situation in

which the number of atoms in higher

energy state is more than that in the lower

energy state.

• At thermal equilibrium, the number of

atoms N2 i.e., the population of atoms at

higher energy state is much lesser than

the population of the atoms at lower

energy state N1 that is N1 > N2.

Page 13: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Conditions of Population

inversion

• There must be at least two energy levels

E2 > E1.

• There must be a source to supply the

energy to the medium.

• The atoms must be continuously raised to

the excited state.

Page 14: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Meta stable States

• Higher energy level – life time is less

• Results spontaneous emission

• population inversion could not be

established

• it is necessary that excited state have a

longer lifetime

• Meta stable state

Page 15: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Principle of Laser action

• Principle - stimulated emission

• Active Medium - medium in which

population inversion can be achieved

• Active Centre - material in which the

atoms are raised to the excited state

• Pumping Action - process to achieve the

population inversion in the medium

• Optical resonator - induce more and more

stimulated transition

Page 16: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Types of Laser

Page 17: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Mind Map

Page 18: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Stimulating questions

1. In which ways LASER light differs from

ordinary light?

2. Why does the photon incident on

metastable state stimulate atom to the

ground state but not to higher energy

state?

Page 19: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

CO2 Molecular gas laser

• It was the first molecular gas laser

developed by Indian born American

scientist Prof. C. K. N. Pillai.

• It is a four level laser and it operates at

10.6 μm in the far IR region. It is a very

efficient laser.

Page 20: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Energy states of CO2 molecules

• A carbon dioxide molecule - carbon atom

at the center with two oxygen atoms

attached, one at both sides.

• exhibits three independent modes of

vibrations.

1.Symmetric stretching mode.

2.Bending mode

3.Asymmetric stretching mode.

Page 21: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Symmetric stretching mode

• carbon atoms are at rest

• oxygen atoms vibrate simultaneously

along the axis of the molecule

Page 22: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Bending mode

• oxygen atoms and carbon atoms vibrate

perpendicular to molecular axis

Page 23: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Asymmetric stretching mode

• oxygen atoms move in one direction while

carbon atoms in the other direction

Page 24: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Principle

• The active medium is a gas mixture of

CO2, N2 and He. The laser transition takes

place between the vibrational states of CO2

molecules.

Page 25: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Construction

• It consists of a quartz tube 5 m long and

2.5 cm in the diameter. This discharge

tube is filled with gaseous mixture of CO2

(active medium), helium and nitrogen with

suitable partial pressures.

• The terminals of the discharge tubes are

connected to a D.C power supply.

• Two concave mirrors one fully reflecting

and the other partially form an optical

resonator.

Page 26: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Working

• The power output from this laser is 10kW

Page 27: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Characteristics

• Type: It is a molecular gas laser.

• Active medium: A mixture of CO2 , N2 and helium or

water vapour is used as active medium

• Pumping method: Electrical discharge method is used for

Pumping action

• Optical resonator: Two concave mirrors form a resonant

cavity

• Power output: The power output from this laser is about

10kW.

• Nature of output: The nature of output may be

continuous wave or pulsed wave.

• Wavelength of output: The wavelength of output is

0.6μm and 10.6μm.

Page 28: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Advantages

• The construction of CO2 laser is simple

• The output of this laser is continuous.

• It has high efficiency

• It has very high output power.

• The output power can be increased by

extending the length of the gas tube.

Page 29: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Disadvantages

• The contamination of oxygen by carbon

monoxide will have some effect on laser action

• The operating temperature plays an important

role in determining the output power of laser.

• The corrosion may occur at the reflecting

plates.

• Accidental exposure may damage our eyes,

since it is invisible (infra red region) to our

eyes.

Page 30: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Applications

• High power CO2 laser finds applications in material

processing, welding, drilling, cutting soldering etc.

• The low atmospheric attenuation (10.6μm makes

CO2 laser suitable for open air communication.

• It is used for remote sensing

• It is used for treatment of liver and lung diseases.

• It is mostly used in neuro surgery and general

surgery.

• It is used to perform microsurgery and bloodless

operations.

Page 31: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Semiconductor Diode laser

• It is specifically fabricated p-n junction

diode. This diode emits laser light when it

is forward biased.

Page 32: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Principle

• When a p-n junction diode is forward

biased, the electrons from n – region and

the holes from the p- region cross the

junction and recombine with each other.

Page 33: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Construction

Page 34: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

• The active medium is a p-n junction diode –

Gallium Arsenide.

• Active centre – p-n junction diode.

• The electrical voltage is applied to the crystal

through the electrode fixed on the upper surface.

• The end faces of the junction diode are well

polished and parallel to each other – optical

resonator

Construction

Page 35: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Working

Page 36: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

• When the PN junction is forward biased - the

electrons and holes are injected into junction

region in considerable concentration.

• The region around the junction contains a large

amount of electrons in the conduction band and a

large amount of holes in the valence band.

• The electrons and holes recombine with each other

and this recombination’s produce radiation in the

form of light.

• When the forward – biased voltage is increased,

more and more light photons are emitted - trigger a

chain of stimulated recombination resulting in the

release of photons in phase.

Working

Page 37: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

• The photons moving at the plane of the junction

travels back and forth by reflection between two

sides placed parallel and opposite to each other

and grow in strength.

• After gaining enough strength, it gives out the laser

beam of wavelength 84000A

Working

Page 38: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Calculate the wavelength of emission from GaAs

semiconductor laser whose band gap energy is 1.44 ev

(plank’s constant is 6.625 x 10-34 Js and charge of an electron

is 1.6 x 10-19 C.

Given data : Band gap energy Eg = 1.44 ev (or) 1.44 x 1.6 x

10-19 Joules.

Solution :

We know Band gap energy (Eg) = h (or) hc/

we can write = hc/Eg

= 6.625 x 10-34 x 3 x 108) / (1.44 x 1.6 x 10-19)

= 8.6263 x 10-7 m

= 8626.3 x 10-10 m

wave length of GaAs laser = 8626.3 oA

Problem

Page 39: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Characteristics• Type: It is a solid state semiconductor laser.

• Active medium: A PN junction diode made from

single crystal of gallium arsenide is used as an

active medium.

• Pumping method: The direct conversion method is

used for pumping action

• Power output: The power output from this laser is

1mW.

• Nature of output: The nature of output is

continuous wave or pulsed output.

• Wavelength of Output: gallium arsenide laser gives

infrared radiation in the wavelength 8300 to

8500oA

Page 40: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Advantages

• It is very small in dimension. The

arrangement is simple and compact.

• It exhibits high efficiency.

• The laser output can be easily increased

by controlling the junction current

• It is operated with lesser power than ruby

and CO2 laser.

• It requires very little auxiliary equipment

• It can have a continuous wave output or

pulsed output.

Page 41: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Disadvantages

• It is difficult to control the mode pattern

and mode structure of laser.

• The output is usually from 5 degree to 15

degree i.e., laser beam has large

divergence.

• Threshold current density is very large

(400A/mm2).

• 5. It has poor coherence and poor stability.

Page 42: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Application

• It is widely used in fiber optic

communication

• It is used to heal the wounds by infrared

radiation

• It is also used as a pain killer

• It is used in laser printers and CD writing

and reading.

Page 43: LASERSarunkumard.yolasite.com/resources/Unit II module 2 and 3.pdf · LASERS Dr D. Arun Kumar Assistant Professor Department of Physical Sciences Bannari Amman Institute of Technology

Thank you…………