SlideShare a Scribd company logo
Lasers and Fiber
optics
What is Laser?
Light Amplification by Stimulated
Emission of Radiation
•A device 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.
Properties of Laser
3
 The light emitted from a laser is monochromatic, that is, it is of one
color/wavelength. In contrast, ordinary white light is a combination of many
colors (or wavelengths) of light.
 Lasers emit light that is highly directional, that is, laser light is emitted as
a relatively narrow beam in a specific direction. Ordinary light, such as
from a light bulb, is emitted in many directions away from the source.
 The light from a laser is said to be coherent, which means that the
wavelengths of the laser light are in phase in space and time. Ordinary
light can be a mixture of many wavelengths.
These three properties of laser light are what can make it more
hazardous than ordinary light. Laser light can deposit a lot of energy
within a small area.
Monochromacity
Nearly monochromatic light
Example:
He-Ne Laser
λ0 = 632.5 nm
Δλ = 0.2 nm
Diode Laser
λ0 = 900 nm
Δλ = 10 nm
Comparison of the wavelengths of red and
blue light
Directionality
Conventional light source Divergence angle (θd)
Beam divergence: θd= β λ /D
β ~ 1 = f(type of light amplitude distribution, definition of beam diameter)
λ = wavelength
D = beam diameter
Coherence
Incoherent light waves Coherent light waves
7
Incandescent vs. Laser Light
1. Many wavelengths
2. Multidirectional
3. Incoherent
1. Monochromatic
2. Directional
3. Coherent
Basic concepts for a laser
• Absorption
• Spontaneous Emission
• Stimulated Emission
• Population inversion
Absorption
•Energy is absorbed by an atom, the electrons are
excited into vacant energy shells.
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
Pumping
•Optical: Uses flashlamps and high-energy light sources (Ruby
Laser)
•Electrical Discharge: application of a potential difference across
the laser medium (He-Ne Laser)
•Inelastic Collisions between Atoms: Atoms exchange energies
with other by in-elastic collisions and gets excited due to
additional absorbed energy. (He-Ne Laser)
•Direct Conversion: Electrical energy is directly converted into
optical energy as LASER beam (Gallium Arsenide
semiconducting Laser)
•Chemical Reaction: Many exothermic reactions provide
essential energy for pumping of atoms.
Two level system
absorption Spontaneous
emission
Stimulated
emission
hn hn
hn
E1
E2
E1
E2
hn =E2-E1
E1
E2
• n1 - the number of electrons of energy E1
• n2 - the number of electrons of energy E2
•Population inversion-
n2>>n1
2 2 1
1
( )
exp
n E E
n kT
 
 
  
 
Boltzmann’s equation
example: T=3000 K E2-E1=2.0
eV
4
2
1
4.4 10
n
n

 
Resonance Cavities
and Longitudinal Modes
Since the wavelengths involved with lasers and
masers spread over small ranges, and are also
absolutely small, most cavities will achieve
lengthwise resonance
Plane
parallel
resonator
Concentric
resonator
Confocal
resonator
Unstable
resonator
Hemispheric
al resonator
Hemifocal
resonator
c
c
f
f
c: center of curvature, f: focal point
L = nλ
Transverse Modes
TEM00:
I(r) = (2P/πd2)*exp(-2r2/d2)
(d is spot size measured
to the 1/e2 points)
Due to boundary conditions and
quantum mechanical wave
equations

More Related Content

PPTX
PPT
LASER FUNDAMENTALS AND OPTICAL FIBER PRINCIPAL
DOCX
LASERS, CHARACTERISTICS, STIMULATED ABSORPTION, SPONTANEOUS EMISSION, STIMULA...
PPTX
Properties-lasermmmmmmmmmmmmmmmmmmm.pptx
PPTX
Laser in electrotherapy ppt by Dr. Mumux
PPT
Light Ampliation by stimulated Emission of Laser
PPTX
Lasers in urology
PPT
Advanced optoelectronics and optical communication
LASER FUNDAMENTALS AND OPTICAL FIBER PRINCIPAL
LASERS, CHARACTERISTICS, STIMULATED ABSORPTION, SPONTANEOUS EMISSION, STIMULA...
Properties-lasermmmmmmmmmmmmmmmmmmm.pptx
Laser in electrotherapy ppt by Dr. Mumux
Light Ampliation by stimulated Emission of Laser
Lasers in urology
Advanced optoelectronics and optical communication

Similar to LASER AND M0DES OF PROPAGATION OF EM WAVE (20)

PPT
LASER_103326.ppt its types classification
PPTX
lasers ppt.pptx
PPT
LASER-Theory.ppt
PPSX
Basic Idea of Laser by deepika gupta
PPT
Physics engineering physics chapter 2 laser Chapter_ 2(Laser).ppt
PPT
Laser and its applications, optical fibres.ppt
PPTX
Optical energy, fluorescence and phosphorescence
PDF
Lecture1(laser).pptx.pdf
PPT
laser-ppt.ppt
PPT
L5.ppt
PPT
Communication - Laser Class 12 Part-7
PPT
Properties of LASER and characteristics.ppt
PPTX
Fundamentals of Laser( Laser physics).pptx
PPT
Laser Systems PPT Theory for Graduatates
PPT
LASER-concepts principle working and Theory.ppt
PPTX
7_laser.pptx for class 12 students cbse board
PPT
7_laser.ppt
PPTX
Laser.pptx
PPT
Lecture-1(Lasersbasics) (1).ppt
PPT
PHYA4-LASERS.ppt, for first year B.E./BTech
LASER_103326.ppt its types classification
lasers ppt.pptx
LASER-Theory.ppt
Basic Idea of Laser by deepika gupta
Physics engineering physics chapter 2 laser Chapter_ 2(Laser).ppt
Laser and its applications, optical fibres.ppt
Optical energy, fluorescence and phosphorescence
Lecture1(laser).pptx.pdf
laser-ppt.ppt
L5.ppt
Communication - Laser Class 12 Part-7
Properties of LASER and characteristics.ppt
Fundamentals of Laser( Laser physics).pptx
Laser Systems PPT Theory for Graduatates
LASER-concepts principle working and Theory.ppt
7_laser.pptx for class 12 students cbse board
7_laser.ppt
Laser.pptx
Lecture-1(Lasersbasics) (1).ppt
PHYA4-LASERS.ppt, for first year B.E./BTech
Ad

Recently uploaded (20)

PPTX
Introduction to Building Materials
PDF
Hazard Identification & Risk Assessment .pdf
PDF
SOIL: Factor, Horizon, Process, Classification, Degradation, Conservation
DOC
Soft-furnishing-By-Architect-A.F.M.Mohiuddin-Akhand.doc
PPTX
Final Presentation General Medicine 03-08-2024.pptx
PDF
احياء السادس العلمي - الفصل الثالث (التكاثر) منهج متميزين/كلية بغداد/موهوبين
PDF
LNK 2025 (2).pdf MWEHEHEHEHEHEHEHEHEHEHE
PDF
RTP_AR_KS1_Tutor's Guide_English [FOR REPRODUCTION].pdf
PPTX
UV-Visible spectroscopy..pptx UV-Visible Spectroscopy – Electronic Transition...
PPTX
UNIT III MENTAL HEALTH NURSING ASSESSMENT
PPTX
1st Inaugural Professorial Lecture held on 19th February 2020 (Governance and...
PPTX
Unit 4 Skeletal System.ppt.pptxopresentatiom
PDF
A GUIDE TO GENETICS FOR UNDERGRADUATE MEDICAL STUDENTS
PPTX
Chinmaya Tiranga Azadi Quiz (Class 7-8 )
PPTX
Cell Types and Its function , kingdom of life
PDF
Practical Manual AGRO-233 Principles and Practices of Natural Farming
PPTX
Introduction-to-Literarature-and-Literary-Studies-week-Prelim-coverage.pptx
PDF
OBE - B.A.(HON'S) IN INTERIOR ARCHITECTURE -Ar.MOHIUDDIN.pdf
PPTX
Radiologic_Anatomy_of_the_Brachial_plexus [final].pptx
PPTX
A powerpoint presentation on the Revised K-10 Science Shaping Paper
Introduction to Building Materials
Hazard Identification & Risk Assessment .pdf
SOIL: Factor, Horizon, Process, Classification, Degradation, Conservation
Soft-furnishing-By-Architect-A.F.M.Mohiuddin-Akhand.doc
Final Presentation General Medicine 03-08-2024.pptx
احياء السادس العلمي - الفصل الثالث (التكاثر) منهج متميزين/كلية بغداد/موهوبين
LNK 2025 (2).pdf MWEHEHEHEHEHEHEHEHEHEHE
RTP_AR_KS1_Tutor's Guide_English [FOR REPRODUCTION].pdf
UV-Visible spectroscopy..pptx UV-Visible Spectroscopy – Electronic Transition...
UNIT III MENTAL HEALTH NURSING ASSESSMENT
1st Inaugural Professorial Lecture held on 19th February 2020 (Governance and...
Unit 4 Skeletal System.ppt.pptxopresentatiom
A GUIDE TO GENETICS FOR UNDERGRADUATE MEDICAL STUDENTS
Chinmaya Tiranga Azadi Quiz (Class 7-8 )
Cell Types and Its function , kingdom of life
Practical Manual AGRO-233 Principles and Practices of Natural Farming
Introduction-to-Literarature-and-Literary-Studies-week-Prelim-coverage.pptx
OBE - B.A.(HON'S) IN INTERIOR ARCHITECTURE -Ar.MOHIUDDIN.pdf
Radiologic_Anatomy_of_the_Brachial_plexus [final].pptx
A powerpoint presentation on the Revised K-10 Science Shaping Paper
Ad

LASER AND M0DES OF PROPAGATION OF EM WAVE

  • 2. What is Laser? Light Amplification by Stimulated Emission of Radiation •A device 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. Properties of Laser 3  The light emitted from a laser is monochromatic, that is, it is of one color/wavelength. In contrast, ordinary white light is a combination of many colors (or wavelengths) of light.  Lasers emit light that is highly directional, that is, laser light is emitted as a relatively narrow beam in a specific direction. Ordinary light, such as from a light bulb, is emitted in many directions away from the source.  The light from a laser is said to be coherent, which means that the wavelengths of the laser light are in phase in space and time. Ordinary light can be a mixture of many wavelengths. These three properties of laser light are what can make it more hazardous than ordinary light. Laser light can deposit a lot of energy within a small area.
  • 4. Monochromacity Nearly monochromatic light Example: He-Ne Laser λ0 = 632.5 nm Δλ = 0.2 nm Diode Laser λ0 = 900 nm Δλ = 10 nm Comparison of the wavelengths of red and blue light
  • 5. Directionality Conventional light source Divergence angle (θd) Beam divergence: θd= β λ /D β ~ 1 = f(type of light amplitude distribution, definition of beam diameter) λ = wavelength D = beam diameter
  • 6. Coherence Incoherent light waves Coherent light waves
  • 7. 7 Incandescent vs. Laser Light 1. Many wavelengths 2. Multidirectional 3. Incoherent 1. Monochromatic 2. Directional 3. Coherent
  • 8. Basic concepts for a laser • Absorption • Spontaneous Emission • Stimulated Emission • Population inversion
  • 9. Absorption •Energy is absorbed by an atom, the electrons are excited into vacant energy shells.
  • 10. 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.
  • 11. Stimulated Emission atoms in an upper energy level can be triggered or stimulated in phase by an incoming photon of a specific energy.
  • 12. 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
  • 13. 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
  • 14. Pumping •Optical: Uses flashlamps and high-energy light sources (Ruby Laser) •Electrical Discharge: application of a potential difference across the laser medium (He-Ne Laser) •Inelastic Collisions between Atoms: Atoms exchange energies with other by in-elastic collisions and gets excited due to additional absorbed energy. (He-Ne Laser) •Direct Conversion: Electrical energy is directly converted into optical energy as LASER beam (Gallium Arsenide semiconducting Laser) •Chemical Reaction: Many exothermic reactions provide essential energy for pumping of atoms.
  • 15. Two level system absorption Spontaneous emission Stimulated emission hn hn hn E1 E2 E1 E2 hn =E2-E1
  • 16. E1 E2 • n1 - the number of electrons of energy E1 • n2 - the number of electrons of energy E2 •Population inversion- n2>>n1 2 2 1 1 ( ) exp n E E n kT          Boltzmann’s equation example: T=3000 K E2-E1=2.0 eV 4 2 1 4.4 10 n n   
  • 17. Resonance Cavities and Longitudinal Modes Since the wavelengths involved with lasers and masers spread over small ranges, and are also absolutely small, most cavities will achieve lengthwise resonance Plane parallel resonator Concentric resonator Confocal resonator Unstable resonator Hemispheric al resonator Hemifocal resonator c c f f c: center of curvature, f: focal point L = nλ
  • 18. Transverse Modes TEM00: I(r) = (2P/πd2)*exp(-2r2/d2) (d is spot size measured to the 1/e2 points) Due to boundary conditions and quantum mechanical wave equations