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Introduction on LASER
› LASER is a acronym for Light Amplification by Stimulated
Emission of Radiation. In Laser the intensity of light is amplified
by a process called stimulated emission.
› The laser is perhaps the most important optical device to be
developed in the past 50 years. Since its arrival in the 1960s, rather
quiet and unheralded outside the scientific community, it has
provided the stimulus to make optics one of the most rapidly
growing fields in science and technology today.
› In 1960, T.H.Maiman built the first laser device (ruby laser).
Within months of the arrival of Maiman’s ruby laser, which
emitted deep red light at a wavelength of 694.3 nm, A. Javan
and associates developed the first gas laser (He-Ne laser), which
emitted light in both the infrared (at 1.15mm) and visible
(at 632.8 nm) spectral regions.
› Following the birth of the ruby and He-Ne lasers, others devices
followed in rapid succession, each with a different laser medium
and a different wavelength emission. For the greater part of the
1960s, the laser was viewed by the world of industry and
technology as scientific curiosity.
Principle of laser
It is based on the principle of stimulated emission of
radiation, with light amplification. For stimulated
emission of radiation to take place, the population of
atoms in higher energy level should be greater than
the lower energy level, i.e., N2>N1 . This can be
achieved by pumping. Light amplification is achieved
by photon multiplication within an optical resonator
cavity.
Characteristics of LASER
The following characteristics, distinguishes a laser beam from an ordinary light.
› Coherence: The wave trains which are identical in phase and direction are
called coherent waves.
› High intensity: Due to the coherent nature of laser, it has ability to focus over
a small area of 10-6
cm2
.
› High directionality: an ordinary light source emits light in all possible
directions. But, laser travels as a parallel beam it can travel over a long
distance without spreading.
› Monochromaticity: The light from a normal monochromatic source spreads
over a range of wavelength of the order 100nm. But, the spread is of 1nm for
laser.
Einstein’s quantum theory of radiation
In 1916, according to Einstein, the interaction of
radiation with matter could be explained in terms
of three basic processes:
1. Induced absorption.
2. Spontaneous Emission.
3. Stimulated Emission.
Spontaneous Emission
It is a process in which there is an emission of a photon whenever an atom transmits
from a higher energy state to a lower energy state without the aid of any external agency.
For this process to take place, the atom has to be in the excited state. Since, the higher
energy level is an unstable one, the excited atom in the higher level E2 spontaneously
returns to the lower energy level E1 with the emission of a photon of a energy hv=E2-E1.
Atom* Atom + Photon
The rate of spontaneous emission of radiation R21 (sp) is proportional to the population
N2 at the higher energy level E2.
Stimulated Emission
It is a process in which there is an emission of a photon whenever an atom transits from a
higher energy level to a lower energy level under the influence of a external agency, i.e., an
inducing photon.
For this process also, the atom should be already in the excited state. Let a photon having an
energy hv=E2-E1 interact with an atom in the excited state. Under such interaction, the incident
photon stimulate the excited atom in the level E2 to transit to the lower energy level E1,
resulting in the emission of a photon of energy hv=E2-E1.
Atom +Photon Atom(Photon + Photon)
The rate of stimulated emission of radiation R21(st) is proportional to the population N2
at the higher energy level E2 and to the density ρof the including photon.
Population Inversion
Population inversion is a state of a achieving more number of atoms in
the excited state compared to the ground state.
i.e., N2 > N1
If the condition is satisfied, then there is more chance for stimulated
emission to take place. Hence, population inversion is an essential
condition for producing laser.
Population inversion can be achieved by a process called pumping.
Pumping
Pumping is the mechanism of exciting atoms from lower energy state to a higher energy state by
supplying energy from an external source. The most commonly used pumping mechanism are,
› Optical pumping: In this type of pumping atoms are excited by means of an external optical
source.
eg: Ruby LASER and Nd:YAG LASER.
› Electrical pumping: In this type of pumping the electrons are accelerated to a high velocity by a
strong electric field. These moving electrons collide with the neutral gas and ionize the
medium. Thus, due to ionization they get raised to a higher energy level.
eg: CO2 LASER.
› Direct conversion: In this type of pumping a direct conversion of electric energy into light takes
place.
eg: Semiconductor LASER.
Applications of LASER
a)In Industry
(1) For welding and melting.
(2) For cutting and drilling holes.
(3) To test the quality of the materials.
b)In Medicine
(1) Used for the treatment of detached retinas.
(2) Used in performing micro and bloodless surgery.
(3) used for the treatment of human and animal cancers
and skin tumors.
c)Military applications
(1) The laser beam can serve as a war weapon.
(2) The laser beam can be used to determine precisely
the distance, velocity and direction from a distant objects
by means of the reflected signal.
d)Science and engineering applications
(1) It is used in fiber optic communication.
(2) It is used in holography.
(3) It is used in underwater communication between
submarines
Laser in physics

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Laser in physics

  • 1.
  • 2.
  • 3. Introduction on LASER › LASER is a acronym for Light Amplification by Stimulated Emission of Radiation. In Laser the intensity of light is amplified by a process called stimulated emission. › The laser is perhaps the most important optical device to be developed in the past 50 years. Since its arrival in the 1960s, rather quiet and unheralded outside the scientific community, it has provided the stimulus to make optics one of the most rapidly growing fields in science and technology today.
  • 4. › In 1960, T.H.Maiman built the first laser device (ruby laser). Within months of the arrival of Maiman’s ruby laser, which emitted deep red light at a wavelength of 694.3 nm, A. Javan and associates developed the first gas laser (He-Ne laser), which emitted light in both the infrared (at 1.15mm) and visible (at 632.8 nm) spectral regions. › Following the birth of the ruby and He-Ne lasers, others devices followed in rapid succession, each with a different laser medium and a different wavelength emission. For the greater part of the 1960s, the laser was viewed by the world of industry and technology as scientific curiosity.
  • 5. Principle of laser It is based on the principle of stimulated emission of radiation, with light amplification. For stimulated emission of radiation to take place, the population of atoms in higher energy level should be greater than the lower energy level, i.e., N2>N1 . This can be achieved by pumping. Light amplification is achieved by photon multiplication within an optical resonator cavity.
  • 6. Characteristics of LASER The following characteristics, distinguishes a laser beam from an ordinary light. › Coherence: The wave trains which are identical in phase and direction are called coherent waves. › High intensity: Due to the coherent nature of laser, it has ability to focus over a small area of 10-6 cm2 . › High directionality: an ordinary light source emits light in all possible directions. But, laser travels as a parallel beam it can travel over a long distance without spreading. › Monochromaticity: The light from a normal monochromatic source spreads over a range of wavelength of the order 100nm. But, the spread is of 1nm for laser.
  • 7. Einstein’s quantum theory of radiation In 1916, according to Einstein, the interaction of radiation with matter could be explained in terms of three basic processes: 1. Induced absorption. 2. Spontaneous Emission. 3. Stimulated Emission.
  • 8. Spontaneous Emission It is a process in which there is an emission of a photon whenever an atom transmits from a higher energy state to a lower energy state without the aid of any external agency. For this process to take place, the atom has to be in the excited state. Since, the higher energy level is an unstable one, the excited atom in the higher level E2 spontaneously returns to the lower energy level E1 with the emission of a photon of a energy hv=E2-E1. Atom* Atom + Photon The rate of spontaneous emission of radiation R21 (sp) is proportional to the population N2 at the higher energy level E2.
  • 9. Stimulated Emission It is a process in which there is an emission of a photon whenever an atom transits from a higher energy level to a lower energy level under the influence of a external agency, i.e., an inducing photon. For this process also, the atom should be already in the excited state. Let a photon having an energy hv=E2-E1 interact with an atom in the excited state. Under such interaction, the incident photon stimulate the excited atom in the level E2 to transit to the lower energy level E1, resulting in the emission of a photon of energy hv=E2-E1. Atom +Photon Atom(Photon + Photon) The rate of stimulated emission of radiation R21(st) is proportional to the population N2 at the higher energy level E2 and to the density ρof the including photon.
  • 10. Population Inversion Population inversion is a state of a achieving more number of atoms in the excited state compared to the ground state. i.e., N2 > N1 If the condition is satisfied, then there is more chance for stimulated emission to take place. Hence, population inversion is an essential condition for producing laser. Population inversion can be achieved by a process called pumping.
  • 11. Pumping Pumping is the mechanism of exciting atoms from lower energy state to a higher energy state by supplying energy from an external source. The most commonly used pumping mechanism are, › Optical pumping: In this type of pumping atoms are excited by means of an external optical source. eg: Ruby LASER and Nd:YAG LASER. › Electrical pumping: In this type of pumping the electrons are accelerated to a high velocity by a strong electric field. These moving electrons collide with the neutral gas and ionize the medium. Thus, due to ionization they get raised to a higher energy level. eg: CO2 LASER. › Direct conversion: In this type of pumping a direct conversion of electric energy into light takes place. eg: Semiconductor LASER.
  • 12. Applications of LASER a)In Industry (1) For welding and melting. (2) For cutting and drilling holes. (3) To test the quality of the materials. b)In Medicine (1) Used for the treatment of detached retinas. (2) Used in performing micro and bloodless surgery. (3) used for the treatment of human and animal cancers and skin tumors.
  • 13. c)Military applications (1) The laser beam can serve as a war weapon. (2) The laser beam can be used to determine precisely the distance, velocity and direction from a distant objects by means of the reflected signal. d)Science and engineering applications (1) It is used in fiber optic communication. (2) It is used in holography. (3) It is used in underwater communication between submarines

Editor's Notes

  1. Imp
  2. Imp 0
  3. This process is responsible for laser action. That is: the stimulated emission of radiation is the principle used in the laser.