7
Most read
8
Most read
9
Most read
PRINCIPLE AND WORKING OF A
SEMICONDUCTOR LASER
COMPILED BY,
ANAND A
ASSISSTANT PROFESSOR
DEPARTMENT OF PHYSICS
ST. JOSEPH’S COLLEGE
TRICHY-620001
Principles of working of a laser
In lasers, photons are interacted in three ways with the
atoms:
1. Absorption of radiation
2. Spontaneous emission
3. Stimulated emission
Absorption of radiation.
Absorption of radiation is the process by which electrons in the ground state absorbs
energy from photons to jump into the higher energy level.
Spontaneous emission.
Spontaneous emission is the process by which electrons in the excited state
return to the ground state by emitting photons.
The electrons in the excited state can stay only for a short period. The time up
to which an excited electron can stay at higher energy state (E2) is known as
the lifetime of excited electrons. The lifetime of electrons in excited state is
10-8 second.
Stimulated emission.
Stimulated emission is the process by which an incoming photon of a specific
frequency can interact with an excited atomic electron causing it to drop to a
lower energy level. In stimulated emission, two photons are emitted (one additional
photon is emitted), one is due to the incident photon and another one is due to the
energy release of excited electron. Thus, two photons are emitted.
Principle and working of a semiconductor laser
INTRODUCTION TO SEMICONDUCTORS
 Semiconductor has conductivity between
conductor and insulator.
 Doping a semiconductor with a small amount
of impurity atoms greatly increases the
number of charge carriers within it.
 When a doped semiconductor contains excess
holes it is called "p-type", and when it contains
excess free electrons it is known as "n-type
Principle and working of a semiconductor laser
 When a p-n junction diode is forward biased, the electrons from n –
region and the holes from the p- region cross the junction and
recombine with each other.
 During the recombination process, the light radiation (photons) is
released from a certain specified direct band gap semiconductors
like Ga-As. This light radiation is known as recombination radiation.
 The photon emitted during recombination stimulates other
electrons and holes to recombine. As a result, stimulated emission
takes place which produces laser.
 The platelet consists of two parts having an electron conductivity (n-type)
and hole conductivity (p-type).
 The photon emission is stimulated in a very thin layer of PN junction (in
order of few microns). The electrical voltage is applied to the crystal
through the electrode fixed on the upper surface.
 The end faces of the junction diode are well polished and parallel to each
other. They act as an optical resonator through which the emitted light
comes out.
 When the PN junction is forward biased with large applied voltage, the
electrons and holes are injected into junction region in considerable
concentration. The region around the junction contains a large amount of
electrons in the conduction band and a large amount of holes in the valence
band.
 If the population density is high, a condition of population inversion is
achieved. The electrons and holes recombine with each other and this
recombination’s produce radiation in the form of light.
When the forward – biased voltage is increased, more and more light
photons are emitted and the light production instantly becomes stronger.
These photons will trigger a chain of stimulated recombination resulting in
the release of photons in phase.
The photons moving at the plane of the junction travels back and forth by
reflection between two sides placed parallel and opposite to each other
and grow in strength.
 After gaining enough strength, it gives out the laser
beam of wavelength 8400o A . The wavelength of
laser light is given by
Where Eg is the band gap energy in joule.
Characteristics
1. Type: It is a solid state semiconductor laser.
2. Active medium: A PN junction diode made from single crystal of gallium arsenide
is used as an active medium.
3. Pumping method: The direct conversion method is used for pumping action
4. Power output: The power output from this laser is 1mW.
5. Nature of output: The nature of output is continuous wave or pulsed output.
6. Wavelength of Output: gallium arsenide laser gives infrared radiation in the
wavelength 8300 to 8500o A .
Advantages
1. It is very small in dimension. The arrangement is simple and compact.
2. It exhibits high efficiency.
3. The laser output can be easily increased by controlling the junction current
4. It is operated with lesser power than ruby and CO2 laser.
5. It requires very little auxiliary equipment
6. It can have a continuous wave output or pulsed output.
Disadvantages
1. It is difficult to control the mode pattern and mode structure of laser.
2. The output is usually from 5 degree to 15 degree i.e., laser beam has
large divergence.
3. The purity and monochromacity are power than other types of laser
4. Threshold current density is very large (400A/mm2).
5. It has poor coherence and poor stability.
Application:
1. It is widely used in fiber optic communication
2. It is used to heal the wounds by infrared radiation
3. It is also used as a pain killer
4. It is used in laser printers and CD writing and reading.
Principle and working of a semiconductor laser

More Related Content

PPTX
Semiconductor laser
PPT
Semiconductor lasers
PPTX
Semicondutor laser
PPTX
LED & LASER sources of light
PPTX
B.tech sem i engineering physics u ii chapter 2-laser
PPTX
Laser diodes
PPTX
Lasers introduction and explanation
PDF
Introduction to Lasers
Semiconductor laser
Semiconductor lasers
Semicondutor laser
LED & LASER sources of light
B.tech sem i engineering physics u ii chapter 2-laser
Laser diodes
Lasers introduction and explanation
Introduction to Lasers

What's hot (20)

PPTX
DOCX
LASERS, CHARACTERISTICS, STIMULATED ABSORPTION, SPONTANEOUS EMISSION, STIMULA...
PPT
Opto electronics devices
PPTX
Avalanche photodiode & there bandwidth
PPTX
Optoelectronics
PPTX
Semiconductor laser
PPT
Photodetector (Photodiode)
PPTX
semiconductor diode laser.pptx
PPTX
Laser diode
PPTX
Laser ppt by jithin m.p,amrita
PPTX
He ne lasers 1
PPT
Semiconductors
PPTX
Conductor semiconductor insulator
PPT
Chap6 photodetectors
PDF
Polarization in Dielectrics | Applied Physics - II | Dielectrics
PPTX
Led (light emitting diode )
PDF
Optical fiber communication Part 2 Sources and Detectors
PPTX
waveguides-ppt
PDF
Two cavity klystron
PPTX
Chapter 4b
LASERS, CHARACTERISTICS, STIMULATED ABSORPTION, SPONTANEOUS EMISSION, STIMULA...
Opto electronics devices
Avalanche photodiode & there bandwidth
Optoelectronics
Semiconductor laser
Photodetector (Photodiode)
semiconductor diode laser.pptx
Laser diode
Laser ppt by jithin m.p,amrita
He ne lasers 1
Semiconductors
Conductor semiconductor insulator
Chap6 photodetectors
Polarization in Dielectrics | Applied Physics - II | Dielectrics
Led (light emitting diode )
Optical fiber communication Part 2 Sources and Detectors
waveguides-ppt
Two cavity klystron
Chapter 4b
Ad

Similar to Principle and working of a semiconductor laser (20)

PPTX
Semiconductor laser by Subhashree behera
PPTX
Solid_ State_ Laser_ Nd_YAG_ Laser.pptx
PPTX
Unit 1. Fundamental of Laser and its applications .pptx
PPTX
Semiconductor Diodes
PPTX
Laser diode fabrication
DOCX
2 ans.docx
PDF
Semiconductor laser by Kunsa Haho of ethiopia
PPTX
PPT
Laser basics
PPTX
Laser matter interaction
PPTX
introduction to laser and introductory concepts
PPT
Communication Engineering LED and LASER Sources.ppt
PPTX
Lasers
PPTX
Laser matter interaction
PDF
physics educationQWASFJLKNMSFD'XB,M,MNFKK;,
PPTX
FEE ppt Yash.pptx
PPTX
OCN_Unit.3.pptx
PPT
Chapter6 optical sources
PPTX
Phy lasers
PDF
Comparison of semiconductor lasers at wavelength 980 nm and 1480 nm using InG...
Semiconductor laser by Subhashree behera
Solid_ State_ Laser_ Nd_YAG_ Laser.pptx
Unit 1. Fundamental of Laser and its applications .pptx
Semiconductor Diodes
Laser diode fabrication
2 ans.docx
Semiconductor laser by Kunsa Haho of ethiopia
Laser basics
Laser matter interaction
introduction to laser and introductory concepts
Communication Engineering LED and LASER Sources.ppt
Lasers
Laser matter interaction
physics educationQWASFJLKNMSFD'XB,M,MNFKK;,
FEE ppt Yash.pptx
OCN_Unit.3.pptx
Chapter6 optical sources
Phy lasers
Comparison of semiconductor lasers at wavelength 980 nm and 1480 nm using InG...
Ad

Recently uploaded (20)

PDF
BIO-INSPIRED ARCHITECTURE FOR PARSIMONIOUS CONVERSATIONAL INTELLIGENCE : THE ...
PPTX
Feature types and data preprocessing steps
PDF
Exploratory_Data_Analysis_Fundamentals.pdf
PDF
Influence of Green Infrastructure on Residents’ Endorsement of the New Ecolog...
PDF
Abrasive, erosive and cavitation wear.pdf
PPTX
tack Data Structure with Array and Linked List Implementation, Push and Pop O...
PPTX
Management Information system : MIS-e-Business Systems.pptx
PPTX
Software Engineering and software moduleing
PDF
ChapteR012372321DFGDSFGDFGDFSGDFGDFGDFGSDFGDFGFD
PPTX
CyberSecurity Mobile and Wireless Devices
PDF
Artificial Superintelligence (ASI) Alliance Vision Paper.pdf
PPTX
AUTOMOTIVE ENGINE MANAGEMENT (MECHATRONICS).pptx
PPT
Total quality management ppt for engineering students
PDF
distributed database system" (DDBS) is often used to refer to both the distri...
PDF
August 2025 - Top 10 Read Articles in Network Security & Its Applications
PPTX
communication and presentation skills 01
PPTX
Fundamentals of Mechanical Engineering.pptx
PDF
Improvement effect of pyrolyzed agro-food biochar on the properties of.pdf
PDF
EXPLORING LEARNING ENGAGEMENT FACTORS INFLUENCING BEHAVIORAL, COGNITIVE, AND ...
PPTX
Current and future trends in Computer Vision.pptx
BIO-INSPIRED ARCHITECTURE FOR PARSIMONIOUS CONVERSATIONAL INTELLIGENCE : THE ...
Feature types and data preprocessing steps
Exploratory_Data_Analysis_Fundamentals.pdf
Influence of Green Infrastructure on Residents’ Endorsement of the New Ecolog...
Abrasive, erosive and cavitation wear.pdf
tack Data Structure with Array and Linked List Implementation, Push and Pop O...
Management Information system : MIS-e-Business Systems.pptx
Software Engineering and software moduleing
ChapteR012372321DFGDSFGDFGDFSGDFGDFGDFGSDFGDFGFD
CyberSecurity Mobile and Wireless Devices
Artificial Superintelligence (ASI) Alliance Vision Paper.pdf
AUTOMOTIVE ENGINE MANAGEMENT (MECHATRONICS).pptx
Total quality management ppt for engineering students
distributed database system" (DDBS) is often used to refer to both the distri...
August 2025 - Top 10 Read Articles in Network Security & Its Applications
communication and presentation skills 01
Fundamentals of Mechanical Engineering.pptx
Improvement effect of pyrolyzed agro-food biochar on the properties of.pdf
EXPLORING LEARNING ENGAGEMENT FACTORS INFLUENCING BEHAVIORAL, COGNITIVE, AND ...
Current and future trends in Computer Vision.pptx

Principle and working of a semiconductor laser

  • 1. PRINCIPLE AND WORKING OF A SEMICONDUCTOR LASER COMPILED BY, ANAND A ASSISSTANT PROFESSOR DEPARTMENT OF PHYSICS ST. JOSEPH’S COLLEGE TRICHY-620001
  • 2. Principles of working of a laser In lasers, photons are interacted in three ways with the atoms: 1. Absorption of radiation 2. Spontaneous emission 3. Stimulated emission
  • 3. Absorption of radiation. Absorption of radiation is the process by which electrons in the ground state absorbs energy from photons to jump into the higher energy level.
  • 4. Spontaneous emission. Spontaneous emission is the process by which electrons in the excited state return to the ground state by emitting photons. The electrons in the excited state can stay only for a short period. The time up to which an excited electron can stay at higher energy state (E2) is known as the lifetime of excited electrons. The lifetime of electrons in excited state is 10-8 second.
  • 5. Stimulated emission. Stimulated emission is the process by which an incoming photon of a specific frequency can interact with an excited atomic electron causing it to drop to a lower energy level. In stimulated emission, two photons are emitted (one additional photon is emitted), one is due to the incident photon and another one is due to the energy release of excited electron. Thus, two photons are emitted.
  • 7. INTRODUCTION TO SEMICONDUCTORS  Semiconductor has conductivity between conductor and insulator.  Doping a semiconductor with a small amount of impurity atoms greatly increases the number of charge carriers within it.  When a doped semiconductor contains excess holes it is called "p-type", and when it contains excess free electrons it is known as "n-type
  • 8. Principle and working of a semiconductor laser  When a p-n junction diode is forward biased, the electrons from n – region and the holes from the p- region cross the junction and recombine with each other.  During the recombination process, the light radiation (photons) is released from a certain specified direct band gap semiconductors like Ga-As. This light radiation is known as recombination radiation.  The photon emitted during recombination stimulates other electrons and holes to recombine. As a result, stimulated emission takes place which produces laser.
  • 9.  The platelet consists of two parts having an electron conductivity (n-type) and hole conductivity (p-type).  The photon emission is stimulated in a very thin layer of PN junction (in order of few microns). The electrical voltage is applied to the crystal through the electrode fixed on the upper surface.  The end faces of the junction diode are well polished and parallel to each other. They act as an optical resonator through which the emitted light comes out.
  • 10.  When the PN junction is forward biased with large applied voltage, the electrons and holes are injected into junction region in considerable concentration. The region around the junction contains a large amount of electrons in the conduction band and a large amount of holes in the valence band.
  • 11.  If the population density is high, a condition of population inversion is achieved. The electrons and holes recombine with each other and this recombination’s produce radiation in the form of light. When the forward – biased voltage is increased, more and more light photons are emitted and the light production instantly becomes stronger. These photons will trigger a chain of stimulated recombination resulting in the release of photons in phase. The photons moving at the plane of the junction travels back and forth by reflection between two sides placed parallel and opposite to each other and grow in strength.
  • 12.  After gaining enough strength, it gives out the laser beam of wavelength 8400o A . The wavelength of laser light is given by Where Eg is the band gap energy in joule.
  • 13. Characteristics 1. Type: It is a solid state semiconductor laser. 2. Active medium: A PN junction diode made from single crystal of gallium arsenide is used as an active medium. 3. Pumping method: The direct conversion method is used for pumping action 4. Power output: The power output from this laser is 1mW. 5. Nature of output: The nature of output is continuous wave or pulsed output. 6. Wavelength of Output: gallium arsenide laser gives infrared radiation in the wavelength 8300 to 8500o A .
  • 14. Advantages 1. It is very small in dimension. The arrangement is simple and compact. 2. It exhibits high efficiency. 3. The laser output can be easily increased by controlling the junction current 4. It is operated with lesser power than ruby and CO2 laser. 5. It requires very little auxiliary equipment 6. It can have a continuous wave output or pulsed output.
  • 15. Disadvantages 1. It is difficult to control the mode pattern and mode structure of laser. 2. The output is usually from 5 degree to 15 degree i.e., laser beam has large divergence. 3. The purity and monochromacity are power than other types of laser 4. Threshold current density is very large (400A/mm2). 5. It has poor coherence and poor stability.
  • 16. Application: 1. It is widely used in fiber optic communication 2. It is used to heal the wounds by infrared radiation 3. It is also used as a pain killer 4. It is used in laser printers and CD writing and reading.

Editor's Notes