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8/7/2019 12369_L7 Laser
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L7LASER
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LASER
LLight
AAmplification by
SStimulated
EEmission of
RRadiation
http://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/L%20is%20for%20Light.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/A%20is%20for%20Amplification.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/S%20is%20for%20Stimulated.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/S%20is%20for%20Stimulated.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/E%20is%20for%20Emission.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/R%20is%20for%20Radiation.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/R%20is%20for%20Radiation.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/R%20is%20for%20Radiation.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/E%20is%20for%20Emission.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/S%20is%20for%20Stimulated.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/A%20is%20for%20Amplification.htmhttp://../01-01-10%20to%2001-06-10/PHY112/Course%20Content/LASER/laser/L%20is%20for%20Light.htm8/7/2019 12369_L7 Laser
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Properties of laser
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Monochromatic
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Directionality
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Coherence
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Incandescent vs. Laser Light
1. Many wavelengths
2. Multidirectional
3. Incoherent
1. Monochromatic
2. Directional
3. Coherent
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BASIC PRINCIPLE NEEDEDFOR LASER
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Stimulated Absorption
Energy is absorbed by an atom, the electrons are
excited into vacant energy shells.
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Spontaneous Emission
The atom decays from level 2 to level 1 through theemission of a photon with the energy hv. It is acompletely random process.
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Stimulated Emission
atoms in an upper energy level can be triggered or
stimulated in phase by an incoming photon of a specific
energy.
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Stimulated Emission
The stimulated photons have unique properties:
In phase with the incident photon
Same wavelength as the incident photon
Travel in same direction as incident photon
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WHY WE NEED META STABLE
STATE?
ANSWER IS
With having the metastable state above the
ground level. Atom reaches the meta stable
state (after first stimulated emission) can
remain there for longer time period. So the
number of atom increases in the meta stable
state. And when these atoms come back to theoriginal ground level it emits laser beam.
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A state of a medium where a higher-lying electronic level has
a higher population than a lower-lying level
POPULATION INVERSION
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The method particle of raising a particle from lower energy stateto higher energy state is called pumping.
TYPES OF PUMPING :
1. Optical pumping
2. Electrical pumping
3. X-ray pumping
4. Chemical pumping
PUMPING
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All lasers have 3 essential components:
A lasing or "gain" medium
A source of energy to excite electrons in the gain medium to high energy
states, referred to as "pump" energy
An optical path which allows emitted photons to oscillate and interfere
constructively as energy is added or "pumped" into the system, ie, a
resonator
LASER COMPONENTS
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LASER ACTION
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Types of Laser
a.According to their sources:
1.Gas Lasers2.Crystal Lasers
3.Semiconductors Lasers
4.Liquid Lasers
a.According to the nature of emission:
1.Continuous Wave
2.Pulsed Laser
a.According to their wavelength:1.Visible Region
2.Infrared Region
3.Ultraviolet Region
4.Microwave RegionX-Ray Region
d. According to different levels 1. 2-level laser
2. 3-level laser
3. 4-level laser
e. According to mode of pumping
1. optical
2. chemical
3. electric discharge4. electrical
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2- Level Laser
h
E1
E2
AbsorptionE1
E2h
Spontaneous
Emission
E1
E2hh h
Stimulated
Emission
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THREE STEP LASER
Stimulated absorption
Spontaneous emission to the metastable state
Stimulated emission from metastable state to ground state.
E2
E1
E0
E2 E1
E1 E0
META STABLESTATE
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4-Level LASER
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PRACTICAL LASERS
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RUBY LASER
Construction
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ENERGY LEVEL IN RUBY
LASER
Energy
4A2
4T2
4T1
2T2
2E
LASING
rapid decay
Cr+
Al2O3
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LASER ACTION IN RUBY
LASER
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HE-NE LASER
Construction
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.
Energy Level Diagram of He-Ne
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Energy Level Diagram of He-Ne cont
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Combined Laser Action
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Emission wavelengths of common
lasers
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APPLICATION S OF LASER
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04/13/11
Not to be Taken LightlyThe Weighty Implications of Laser Technology
Applications of
Laser
Technology
Medical
Entertainment
Telecommunications
Military
Optical SurgeryGeneral Surgery Tattoo removal
CD Players DVD Players Video Game Systems
Information tech. Holograms
Weapons
Satellites
Radar
Industry
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04/13/11
Can You See the Light?
Dentists use
laser drills
Bad eyesight can be
corrected by optical
surgery using lasers
CD-Audio is
read by a laser
Tattoo removal is
done using lasers
Cd-Rom discs
are read by lasers
Laser pointers can
enhance
presentations Bar codes in
grocery stores are
scanned by lasers
Video game systems such as
PlayStation 2 utilize lasers
DVD players read
DVDs using lasers
Airplanes areequipped with
laser radar
Military and Spaceaircraft are equipped
with laser guns
Laser tech. is used in printers,
copiers, and scanners
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Einsteins Coefficients
Einstein gives a probability that stimulated
emission is same as absorption.
Means that if a stimulated absorption can
occur then there is same probability that
stimulated emission can occur.
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Equilibrium condition
In case of energy states the number of electron
absorbed and emitted should be equal or the
rate of change of numbers of atoms in two
states should be equal.
0=dt
dN
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Plancks Radiation Law
( )
1
18
3
3
= kTh
ec
hE
Planks gives the formula that howa gas radiate energy.
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Spontaneous emission
A21
:- correspond to spontaneous emission
probability per unit time
This particular emission can occur
without the presence of external field
E(v)
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Stimulated Absorption
B12
:- correspond to stimulated absorption
probability per unit time
This type of absorption can occur in
presence of external field E(v) only
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Stimulated Emission
B21
:- correspond to stimulated emission
probability per unit time
This type of emission can occur in presence of
external field E(v) only
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Total Emission Probability
Spontaneous Emission + Stimulated Emission
A21 + B21 E(v)
Number of atoms that can jump from level E2 to E1 is
( )[ ] 22121 NEBA +
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Total Absorption Probability
( )[ ] 112 NEB
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At Equilibrium
Then
02 =dt
dN
( ) ( )[ ] 22121112 NEBANEB +=
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Emission and absorption are same
( )
=
B
B
N
NB
A
E
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Maxwell Bolzman Distribution
KT
E
eNN
1
01
=
KT
E
eNN
2
02
=
In thermal equilibrium
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So the equations become
kT
h
eN
N
=2
1
So equation becomes
( )1
1
21
1221
21
=B
Be
B
A
EkT
h
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Conclusions
Stimulated emission have same probability as
stimulated absorption
Ratio between spontaneous and stimulated
emission varies with v3
All we need is to calculate one of the
probability to find others.
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THANKS SEE YOU IN NEXTLECTURE