Laser Technology: Principles, Applications, and Einstein's Coefficients

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LASER
LASER
&
&
IT’S APPLICATIONS
IT’S APPLICATIONS
(CO-4 Part-I)
 
 
Dr. Prabodh Sahai Saxena
Prof & Head
Deptt of Physics
LNCT BHOPAL
 
Introduction of laser
Principle of laser
Einstein’s coefficients
Main components of laser
Importance of third energy level
Types of lasers
 
 
The word 
laser
 is an acronym that stands for “light
amplification by the stimulated emission of
radiation”.
Lasers are essentially have following 
characteristics
-
highly directional,
highly intense,
highly monochromatic &
highly coherent optical  light source.
 
 
Introduction
Introduction
 
Laser based on the principle of stimulated emission.
Stimulated emission was postulated by Einstein as
early as in 1917.
In 1960, a solid state Ruby laser is developed by
Maiman on this principle.
In 1961, a gas state He-Ne laser is developed by Ali
Javan and others in Bell telephone laboratory.
 
Principle of Laser
Principle of Laser
 
Absorption of Radiation
Absorption of Radiation
 
Spontaneous Emission of Radiation
Spontaneous Emission of Radiation
 
Stimulated Emission of Radiation
Stimulated Emission of Radiation
 
Einstein’s coefficients are of three types.
coefficient of Absorption (B
12
):
    
P
12
=B
12
u(
ν
)
coefficient of Spontaneous emission (A
21
):
    
P
21
=A
21
coefficient of Stimulated emission (B
21
):
    
P
21
= B
21
u(
ν
)
Where 
u(
ν
)=Energy density of the radiation
 
 
If A
21 
& B
21
 are the coefficient of spontaneous & stimulated
emission respectively, then
    
A
21
/B
21
 = 8
π
h
ν
3
/c
3
Where c=3
˟
10
8
 m/sec=velocity of light
Which conclude that probability of spontaneous emission
increase rapidly with energy difference( E
2
-E
1
=h
ν
) between
two states.
 
Population Inversion
Population Inversion
:-This is the state in which larger
number of atoms in the higher energy level than that
the lower energy level.
     
N
2
>>N
1
Pumping
Pumping
:- 
:- 
The process of achieving population
inversion  is known as pumping. Most  commonly
used methods are as follows.
 
Optical Pumping- (used in Ruby/NdYAG Laser)
 
Electric Discharge (used in He- Ne Laser)
 
Chemical reaction (used in CO
2
 Laser)
 
Direct conversion (In semi conductor Laser)
 
Energy Source
Energy Source
:- It is used to raise the system to an
excited state.
Active Medium
Active Medium
:- This is the material in which
population inversion achieves. This may be solid,
liquid  or gas.
   
for example- In He-Ne Laser mixer of He-Ne gas, in Ruby
laser ruby crystal, in NdYAG laser NdYAG crystal, in CO
2
laser CO
2
 gas is active medium.
Optical Resonator 
Optical Resonator 
:- It consists of two mirrors facing
each other. The active medium is enclosed by this
cavity. One of the mirror is fully reflecting while
other mirror is partially transparent.
 
 
With two energy levels rate of stimulated emission
will equal to the rate of induced absorption.
Therefore, condition of population inversion will not
take place and laser amplification will not occur. So,
third energy level is necessary for laser action. This is
known as metastable state.
 
 
 
Metastable state
Metastable state
:- It is a long lived energy state
(10
-3
 sec) in which atom can stay longer time as
compared to excited energy state. It is exist above the
ground energy state. This is necessary to achieve
population inversion.
 
Among the various kinds of lasers some
important types of lasers are listed below:
Solid state laser : Ruby laser, NdYAG Laser
Gas laser : He-Ne laser, Co
2
 laser
Liquid laser : Europium chelate laser
Dye laser : Courmarin dye laser
Semiconductor laser : Inp laser
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Exploring the fascinating world of lasers, this content delves into the principles governing laser technology, including the concept of stimulated emission by Einstein. It covers the characteristics of lasers, different types, and the significant contributions of pioneers in the field. The explanation of absorption, spontaneous emission, and stimulated emission of radiation, along with Einstein's coefficients, sheds light on the intricate workings of lasers. The importance of energy levels and the rapid increase in the probability of spontaneous emission with energy difference are also discussed.

  • Laser technology
  • Principles
  • Applications
  • Einsteins Coefficients
  • Stimulated emission
  • Energy levels

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  1. LASER & IT S APPLICATIONS (CO-4 Part-I) Dr. Prabodh Sahai Saxena Prof & Head Deptt of Physics LNCT BHOPAL

  2. Introduction of laser Principle of laser Einstein s coefficients Main components of laser Importance of third energy level Types of lasers

  3. Introduction The word laser is an acronym that stands for light amplification by the stimulated emission of radiation . Lasers are essentially have following characteristics- highly directional, highly intense, highly monochromatic & highly coherent optical light source.

  4. Laser based on the principle of stimulated emission. Stimulated emission was postulated by Einstein as early as in 1917. In 1960, a solid state Ruby laser is developed by Maiman on this principle. In 1961, a gas state He-Ne laser is developed by Ali Javan and others in Bell telephone laboratory.

  5. Principle of Laser

  6. Absorption of Radiation

  7. Spontaneous Emission of Radiation

  8. Stimulated Emission of Radiation

  9. Einsteins coefficients are of three types. coefficient of Absorption (B12): P12=B12u( ) coefficient of Spontaneous emission (A21): P21=A21 coefficient of Stimulated emission (B21): P21= B21u( ) Where u( )=Energy density of the radiation

  10. If A21 & B21 are the coefficient of spontaneous & stimulated emission respectively, then A21/B21 = 8 h 3/c3 Where c=3 108 m/sec=velocity of light Which conclude that probability of spontaneous emission increase rapidly with energy difference( E2-E1=h ) between two states.

  11. Population Inversion:-This is the state in which larger number of atoms in the higher energy level than that the lower energy level. N2>>N1 Pumping:- The process of achieving population inversion is known as pumping. Most commonly used methods are as follows. Optical Pumping- (used in Ruby/NdYAG Laser) Electric Discharge (used in He- Ne Laser) Chemical reaction (used in CO2 Laser) Direct conversion (In semi conductor Laser)

  12. Energy Source:- It is used to raise the system to an excited state. Active Medium:- This is the material in which population inversion achieves. This may be solid, liquid or gas. for example- In He-Ne Laser mixer of He-Ne gas, in Ruby laser ruby crystal, in NdYAG laser NdYAG crystal, in CO2 laser CO2 gas is active medium. Optical Resonator :- It consists of two mirrors facing each other. The active medium is enclosed by this cavity. One of the mirror is fully reflecting while other mirror is partially transparent.

  13. With two energy levels rate of stimulated emission will equal to the rate of induced absorption. Therefore, condition of population inversion will not take place and laser amplification will not occur. So, third energy level is necessary for laser action. This is known as metastable state. Metastable state:- It is a long lived energy state (10-3 sec) in which atom can stay longer time as compared to excited energy state. It is exist above the ground energy state. This is necessary to achieve population inversion.

  14. Among the various kinds of lasers some important types of lasers are listed below: Solid state laser : Ruby laser, NdYAG Laser Gas laser : He-Ne laser, Co2 laser Liquid laser : Europium chelate laser Dye laser : Courmarin dye laser Semiconductor laser : Inp laser

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