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B Y
P R O F . S D
LASERS
What is LASER????
Light Amplification by Stimulated Emission of
Radiation
• A device that produces a coherent beam of optical
radiation by stimulating electronic, ionic, or
molecular transitions to higher energy levels.
• When they return to lower energy levels by
stimulated emission, they emit energy.
Basic concepts for a laser
 Absorption
 Spontaneous Emission
 Stimulated Emission
 Population inversion
Lasers: Basic Principle
Absorption and Radiation Processes
Absorption
An electron in an atom can be excited from an energy level E1 to a
higher energy level E2 by absorption:
photon absorption─ hν = E2 – E1.
h
E
E 1
2 


Spontaneous Emission
The atom decays from level 2 to level 1 through the
emission of a photon with the energy hv. It is a completely
random process.
Stimulated Emission
Atoms in an upper energy level can be triggered or stimulated
in phase by an incoming photon of a specific energy.
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
Population Inversion
 A state in which a substance
has been energized, or
excited to specific energy
levels.
 More atoms or molecules are
in a higher excited state.
 The process of producing a
population inversion is
called pumping.
 Examples:
→by lamps of appropriate
intensity
→by electrical discharge
Metastable states
 An atom or molecule in an excited state remains
there for a certain time called the lifetime of that
state, before making a transition to a lower state. The
lifetime of a state is characteristic of the energy level
and varies over a wide range. Most of the states have
a short lifetime, of the order of 10-8 s. However, some
energy states have very long lifetime of the order of
10-3 s or higher. Energy states with such long life
times are called meta-stable states.
Pumping
 The population inversion can be achieved by exciting the
medium with suitable form of energy. This process is called
Pumping.
 There are several methods of pumping a laser and
producing population inversion necessary for the
occurrence of stimulated emission :
(a) Optical pumping
(b) Electric Discharge
(c) Inelastic atom-atom collision
(d) Direct Conversion
(e) Chemical reactions
Characteristics of Laser Beam
 High directionality:
Directionality is the characteristic of laser light that causes it to travel
in a single direction with a narrow cone of divergence. It is defined in
terms of divergence angle.
Divergence angle is twice the angle made by the outer edge with the
axis of the beam.
The angular spread of beam on one side of the axis :
d


 
High Intensity
The intensity of light is defined as the energy passing per unit area per
second through a point normal to the direction of flow. For a spherical
source with output power P , intensity at a point distant r from the source
is given as:
Laser beam is highly intense because it emits light as a narrow beam and
intensity remains high even at large distance from the source.
2
4 r
P
I


Extraordinary monochromacity
If ∆ν is the frequency of a spectral line of frequency ν0then the degree of
monochromacity is defined as:
ε=∆ν/ν0
Smaller is the value of ε, higher is the monochromacity of light.
For laser source ε=10-12 while for ordinary source ε≈10-5
High Coherence
Degree of coherence is the measure of phase correlation in the radiation field
at different locations and different time.
Incoherent
Coherent

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Lecture-1(Lasersbasics) (1).ppt

  • 1. B Y P R O F . S D LASERS
  • 2. What is LASER???? Light Amplification by Stimulated Emission of Radiation • A device that produces a coherent beam of optical radiation by stimulating electronic, ionic, or molecular transitions to higher energy levels. • When they return to lower energy levels by stimulated emission, they emit energy.
  • 3. Basic concepts for a laser  Absorption  Spontaneous Emission  Stimulated Emission  Population inversion
  • 4. Lasers: Basic Principle Absorption and Radiation Processes
  • 5. Absorption An electron in an atom can be excited from an energy level E1 to a higher energy level E2 by absorption: photon absorption─ hν = E2 – E1. h E E 1 2   
  • 6. Spontaneous Emission The atom decays from level 2 to level 1 through the emission of a photon with the energy hv. It is a completely random process.
  • 7. Stimulated Emission Atoms in an upper energy level can be triggered or stimulated in phase by an incoming photon of a specific energy.
  • 8. 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
  • 9. Population Inversion  A state in which a substance has been energized, or excited to specific energy levels.  More atoms or molecules are in a higher excited state.  The process of producing a population inversion is called pumping.  Examples: →by lamps of appropriate intensity →by electrical discharge
  • 10. Metastable states  An atom or molecule in an excited state remains there for a certain time called the lifetime of that state, before making a transition to a lower state. The lifetime of a state is characteristic of the energy level and varies over a wide range. Most of the states have a short lifetime, of the order of 10-8 s. However, some energy states have very long lifetime of the order of 10-3 s or higher. Energy states with such long life times are called meta-stable states.
  • 11. Pumping  The population inversion can be achieved by exciting the medium with suitable form of energy. This process is called Pumping.  There are several methods of pumping a laser and producing population inversion necessary for the occurrence of stimulated emission : (a) Optical pumping (b) Electric Discharge (c) Inelastic atom-atom collision (d) Direct Conversion (e) Chemical reactions
  • 12. Characteristics of Laser Beam  High directionality: Directionality is the characteristic of laser light that causes it to travel in a single direction with a narrow cone of divergence. It is defined in terms of divergence angle. Divergence angle is twice the angle made by the outer edge with the axis of the beam. The angular spread of beam on one side of the axis : d    
  • 13. High Intensity The intensity of light is defined as the energy passing per unit area per second through a point normal to the direction of flow. For a spherical source with output power P , intensity at a point distant r from the source is given as: Laser beam is highly intense because it emits light as a narrow beam and intensity remains high even at large distance from the source. 2 4 r P I  
  • 14. Extraordinary monochromacity If ∆ν is the frequency of a spectral line of frequency ν0then the degree of monochromacity is defined as: ε=∆ν/ν0 Smaller is the value of ε, higher is the monochromacity of light. For laser source ε=10-12 while for ordinary source ε≈10-5
  • 15. High Coherence Degree of coherence is the measure of phase correlation in the radiation field at different locations and different time. Incoherent Coherent