This document provides a summary of different laser types, including He-Ne lasers, injection lasers, Nd-YAG lasers, and dye lasers. It discusses the construction, working principles, and energy diagrams of each laser. The He-Ne laser was the first continuous laser and uses a mixture of helium and neon gases as its active medium. Injection lasers use a semiconductor PN junction as the active medium and achieve population inversion through carrier injection. Nd-YAG lasers use a neodymium-doped yttrium aluminum garnet crystal as the active medium and operate as a four-level laser system. Dye lasers can be widely tuned by changing the organic dye solution
Semiconductor lasers use stimulated emission of radiation to produce coherent laser light. They rely on achieving population inversion in a semiconductor material such as gallium arsenide, where more electrons are in a higher energy state than a lower state. When the electrons drop to the lower state, they emit photons that stimulate the emission of more photons, producing a laser beam. Semiconductor lasers come in homojunction and heterojunction types, and are constructed from layers of doped semiconductor materials to form a p-n junction. Applying a forward voltage bias injects electrons and holes, achieving population inversion and laser action.
The document provides an overview of photonic light sources, specifically LEDs and lasers. It discusses:
1) How LEDs work by emitting photons when electrons fall from a higher to lower energy level within a semiconductor, causing light. The color depends on the energy level difference.
2) The principle of lasers, which involves stimulating emission of radiation to achieve population inversion and optical gain, allowing for amplification of photons within the laser medium.
3) How a laser diode works by achieving population inversion through forward biasing of a p-n junction, allowing stimulated emission and optical feedback via mirrors to produce coherent, collimated light amplification.
The attached narrated power point presentation attempts to explain the working principle of lasers as sources for optical communications. The material will be useful for KTU final year B Tech students who prepare for the subject EC 405, Optical Communications.
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solidRai University
This document provides an overview of band theory of solids. It discusses key concepts such as effective mass of electrons, the concept of holes, and the energy band structure of conductors, semiconductors and insulators. It explains that conductors have overlapping valence and conduction bands, semiconductors have a small bandgap, and insulators have a large bandgap. The document also covers intrinsic and extrinsic semiconductors, the operation of p-n junction diodes under reverse and forward bias, and types of diodes such as simple diodes and Zener diodes.
This document discusses the operation of semiconductor laser diodes. It begins by explaining the basic principles of laser diodes, including how they require an optical cavity to facilitate feedback and generate stimulated emission. It then describes the specific components and mechanisms of common laser diode structures like fundamental, double heterostructure, and buried heterostructure designs. Key points covered include how carrier and photon confinement are achieved to lower threshold currents, the role of optical modes, and factors that determine the laser diode output spectrum.
The document summarizes the principles and working of a semiconductor laser, explaining that it uses stimulated emission from a p-n junction diode made of gallium arsenide to produce coherent infrared laser light, and that applying a forward voltage bias injects electrons and holes to achieve population inversion and trigger stimulated recombination of photons within the diode's optical resonator structure. Semiconductor lasers have applications in fiber optic communication, wound healing, laser printing, and CD/DVD reading/writing due to their compact size, high efficiency, and ability to produce continuous or pulsed laser output.
1. The document discusses the principles and operation of pn-junction diodes and light emitting diodes (LEDs). It describes how a depletion region forms around the pn-junction due to diffusion of holes and electrons.
2. In an LED, electron-hole pair recombination in the depletion region and surrounding areas results in photon emission. The photon energy is approximately equal to the semiconductor's band gap energy.
3. Common LED materials use direct bandgap III-V semiconductors like GaAs and GaP or their alloys. The bandgap can be tuned to emit light across the visible and infrared spectra. Proper device design and encapsulation helps extract more light from the LED.
Semiconductor lasers operate based on stimulated emission of radiation from a semiconductor material. When a semiconductor is forward biased, electrons from the n-type region combine with holes in the p-type region and release energy in the form of photons. These photons stimulate additional electrons to release photons of the same frequency, resulting in coherent laser emission. Semiconductor lasers can be homojunction lasers made of the same semiconductor material on both sides or heterojunction lasers made of different materials on each side. They have applications in optical storage, laser printing, barcode scanners, and fiber optic communication due to their small size, efficiency and ability to be integrated with other devices.
Semiconductor lasers use stimulated emission of radiation to produce coherent laser light. They rely on achieving population inversion in a semiconductor material such as gallium arsenide, where more electrons are in a higher energy state than a lower state. When the electrons drop to the lower state, they emit photons that stimulate the emission of more photons, producing a laser beam. Semiconductor lasers come in homojunction and heterojunction types, and are constructed from layers of doped semiconductor materials to form a p-n junction. Applying a forward voltage bias injects electrons and holes, achieving population inversion and laser action.
The document provides an overview of photonic light sources, specifically LEDs and lasers. It discusses:
1) How LEDs work by emitting photons when electrons fall from a higher to lower energy level within a semiconductor, causing light. The color depends on the energy level difference.
2) The principle of lasers, which involves stimulating emission of radiation to achieve population inversion and optical gain, allowing for amplification of photons within the laser medium.
3) How a laser diode works by achieving population inversion through forward biasing of a p-n junction, allowing stimulated emission and optical feedback via mirrors to produce coherent, collimated light amplification.
The attached narrated power point presentation attempts to explain the working principle of lasers as sources for optical communications. The material will be useful for KTU final year B Tech students who prepare for the subject EC 405, Optical Communications.
Diploma sem 2 applied science physics-unit 3-chap-1 band theory of solidRai University
This document provides an overview of band theory of solids. It discusses key concepts such as effective mass of electrons, the concept of holes, and the energy band structure of conductors, semiconductors and insulators. It explains that conductors have overlapping valence and conduction bands, semiconductors have a small bandgap, and insulators have a large bandgap. The document also covers intrinsic and extrinsic semiconductors, the operation of p-n junction diodes under reverse and forward bias, and types of diodes such as simple diodes and Zener diodes.
This document discusses the operation of semiconductor laser diodes. It begins by explaining the basic principles of laser diodes, including how they require an optical cavity to facilitate feedback and generate stimulated emission. It then describes the specific components and mechanisms of common laser diode structures like fundamental, double heterostructure, and buried heterostructure designs. Key points covered include how carrier and photon confinement are achieved to lower threshold currents, the role of optical modes, and factors that determine the laser diode output spectrum.
The document summarizes the principles and working of a semiconductor laser, explaining that it uses stimulated emission from a p-n junction diode made of gallium arsenide to produce coherent infrared laser light, and that applying a forward voltage bias injects electrons and holes to achieve population inversion and trigger stimulated recombination of photons within the diode's optical resonator structure. Semiconductor lasers have applications in fiber optic communication, wound healing, laser printing, and CD/DVD reading/writing due to their compact size, high efficiency, and ability to produce continuous or pulsed laser output.
1. The document discusses the principles and operation of pn-junction diodes and light emitting diodes (LEDs). It describes how a depletion region forms around the pn-junction due to diffusion of holes and electrons.
2. In an LED, electron-hole pair recombination in the depletion region and surrounding areas results in photon emission. The photon energy is approximately equal to the semiconductor's band gap energy.
3. Common LED materials use direct bandgap III-V semiconductors like GaAs and GaP or their alloys. The bandgap can be tuned to emit light across the visible and infrared spectra. Proper device design and encapsulation helps extract more light from the LED.
Semiconductor lasers operate based on stimulated emission of radiation from a semiconductor material. When a semiconductor is forward biased, electrons from the n-type region combine with holes in the p-type region and release energy in the form of photons. These photons stimulate additional electrons to release photons of the same frequency, resulting in coherent laser emission. Semiconductor lasers can be homojunction lasers made of the same semiconductor material on both sides or heterojunction lasers made of different materials on each side. They have applications in optical storage, laser printing, barcode scanners, and fiber optic communication due to their small size, efficiency and ability to be integrated with other devices.
Solid State Electronics.
this slide is made from taking help of
TextBook
Ben.G.StreetmanandSanjayBanerjee:SolidStateElectronicDevices,Prentice-HallofIndiaPrivateLimited.
Nature and the characteristics of semi conductors(diodes and dopedWilson Jimmy
Group IV elements like silicon and germanium are semiconductors that have electrical conductivity between conductors and insulators. Their properties can be modified through doping, which involves adding small amounts of impurities. Doping silicon with elements having five valence electrons (like phosphorus) creates an n-type semiconductor with free electrons. Doping with elements having three valence electrons (like boron) creates a p-type semiconductor with holes. Placing a p-type and n-type semiconductor together forms a diode, which allows current to flow easily in only one direction.
1. A light emitting diode (LED) is a p-n junction diode that emits light when forward biased as electrons and holes recombine and release energy as photons.
2. The energy conversion in an LED occurs in two stages: carriers in the semiconductor absorb electrical energy raising them above equilibrium value, and most carriers give up this energy as spontaneous photon emission when they recombine.
3. The wavelength of light emitted by an LED depends on the bandgap of the semiconductor material, with lower bandgap materials emitting infrared light and higher bandgap materials emitting visible light.
The document summarizes key concepts in optics and optical properties of materials. It discusses topics like electromagnetic radiation spectrum, optical classifications of materials as transparent, translucent or opaque. It also covers concepts like reflection, refraction, absorption, transmission and how they relate to the band structure and band gaps of materials. Specific phenomena like fluorescence, phosphorescence, photoelasticity and their working principles are defined. Applications of optics like lasers, optical data storage are also briefly mentioned.
This document discusses the interactions between x-rays and matter. There are three main interactions - photoelectric effect, Compton scattering, and coherent scattering. The photoelectric effect occurs when a photon ejects an inner shell electron from an atom. This produces characteristic x-rays and leaves the atom ionized. Compton scattering involves the deflection of photons by outer shell electrons, producing scattered radiation. At diagnostic energies, Compton scattering is the most common interaction. The photoelectric effect dominates for high atomic number materials and low energy x-rays. These two interactions are most important in diagnostic radiology, while coherent scattering, pair production and photodisintegration occur at higher energies.
Basic of semiconductors and optical propertiesKamran Ansari
This presentation explains the band structure, intrinsic semiconductor, extrinsic semiconductor, electrical conductivity, mobility, hall effect, p-n junction diode, tunnel diode and optical properties of the semiconductor.
The document describes the operation of pn-junction and pin photodiodes. Pn-junction photodiodes convert light to electrical signals by separating electron-hole pairs generated by photon absorption in the depletion region. The quantum efficiency and responsivity characterize a photodiode's performance. Pin photodiodes have wider depletion widths than pn-junctions, allowing detection at higher frequencies and wavelengths. The intrinsic region in pin diodes provides a uniform electric field for carrier separation and drift, improving efficiency.
There are four main types of electrical polarization mechanisms: electronic, ionic, orientation, and space charge polarization. Electronic polarization occurs when an external electric field causes the nucleus and electron cloud of an atom to displace slightly, inducing a dipole moment. Ionic polarization is similar but occurs in ionic compounds due to displacement of ions from their equilibrium positions. Orientation polarization results from permanent molecular dipoles rotating to align with an applied field. Space charge polarization involves accumulation of charges at interfaces in dielectric materials when an electric field is applied. The total polarization of a material is generally the sum of these different polarization contributions.
1. The document discusses optical properties of semiconductors when exposed to electromagnetic radiation like light.
2. It explains concepts like absorption, reflection, transmission and emission spectra that can be obtained from materials and how they provide information about electronic band structures.
3. Key optical phenomena discussed include photon absorption promoting electrons from the valence to conduction band if the photon energy exceeds the semiconductor bandgap, and the interaction of light with materials leading to processes like reflection, refraction, scattering and dispersion.
X-rays can interact with matter through three main processes: the photoelectric effect, Compton effect, and pair production. The photoelectric effect occurs when an incoming photon ejects an inner shell electron. The ejected electron has kinetic energy and can ionize other atoms. The Compton effect happens when a photon collides with and ejects an outer shell electron. This produces a scattered photon and ejected electron. The probability of these interactions depends on factors like the photon energy and material's atomic number. High atomic number materials are stronger absorbers of x-rays via the photoelectric effect.
The document discusses the structure of atoms and the electromagnetic spectrum. It describes how atoms are made up of a nucleus surrounded by electrons in specific orbits. The electromagnetic spectrum is produced when charged particles accelerate and electromagnetic radiation travels as waves and particles. The different types of electromagnetic radiation are classified based on their wavelength, from long radio waves to short gamma rays.
The document discusses the mechanism behind photon emission in LEDs. It begins by explaining that in direct bandgap semiconductors, electron-hole recombination can directly produce photons without changing momentum. This allows efficient light emission. It then describes how different semiconductors like GaN, GaAsP, and GaP can be used to produce LEDs across the visible spectrum through modification of their bandgaps. The document concludes by discussing challenges in producing efficient blue LEDs and prospects for overcoming them.
1. LASER stands for 'Light Amplification by Stimulated Emission of Radiation'. It produces a very intense, concentrated, highly parallel and monochromatic beam of light.
2. Coherence is an important property of laser light. Ordinary light sources produce incoherent light with a wide range of frequencies, while laser produces coherent light that is uniform in frequency, amplitude, continuity and constant initial phase difference.
3. Population inversion is achieved by pumping atoms to a higher energy metastable state such that more atoms are in the excited state than the lower energy state. This allows for stimulated emission to overtake absorption, leading to amplification of light in the laser medium.
This document discusses semiconductor materials and devices. It begins by explaining electricity and electron bands in atoms. It then discusses the properties and atomic structures of conductors, insulators, and semiconductors. Semiconductors can be made to act as insulators or conductors through doping, which introduces impurity atoms. The document describes how n-type and p-type semiconductors are formed and their current flow. It concludes by explaining how a p-n junction diode is formed at the interface of p-type and n-type semiconductors and its current-voltage characteristics.
This document discusses semiconductor materials and their properties. It covers elemental and compound semiconductors, including gallium nitride used in LEDs. It describes the band structure of semiconductors including the valence and conduction bands separated by the bandgap. Carrier generation and recombination processes are explained. Intrinsic and extrinsic semiconductors are defined based on their carrier concentrations.
The document discusses the electro-optical properties of semiconductors under an applied electric field. It describes the Franz-Keldysh effect where an electric field causes a red shift and broadening of the band edge absorption in bulk semiconductors. It also discusses the Stark effect which modifies the excitonic absorption due to changes in the electron-hole interaction. When applied to quantum wells, the electric field can cause a quantum-confined Stark effect or quantum-confined Franz-Keldysh effect, broadening excitonic resonances and allowing forbidden transitions.
This document provides an overview of electrical properties of materials. It discusses how electrons move in different materials and the relationship between carrier density and mobility. Metals are good conductors due to their high number of free electrons. Semiconductors and insulators have lower conductivity since electrons must jump across a band gap. The document outlines band theory, explaining how energy bands arise from the interaction of atomic orbitals. Metals have partially filled or overlapping bands, allowing conduction, while semiconductors and insulators have filled valence bands separated from empty conduction bands by a band gap. Electrical properties depend on carrier concentration and mobility, with metals having high values of both.
Semiconductors have electrical properties between conductors and insulators. They behave as insulators at low temperatures but conduct electricity at room temperature due to their small band gap. Doping semiconductors with impurities creates an excess of electrons or holes, making them n-type or p-type. A p-n junction is formed at the boundary between p-type and n-type semiconductors and allows current to flow in only one direction, making it useful for diodes. Diodes are used to convert alternating current to direct current and have many applications in electronics.
Semiconductors have electrical properties between conductors and insulators. They conduct electricity better than insulators but not as well as metals. Semiconductors have small energy band gaps allowing electrons to move between valence and conduction bands with small amounts of energy. Semiconductors can be made intrinsic, with no impurities, or extrinsic through doping with elements from groups III/V. N-type doping adds free electrons while P-type adds holes. Intrinsic semiconductors have equal numbers of electrons and holes while extrinsic have more of one carrier type. Common semiconductors include silicon and germanium which have diamond cubic crystal structures.
Interaction of xrays and gamma rays with matter iiSneha George
The document discusses four main mechanisms by which photons interact with matter: coherent scattering, photoelectric effect, Compton scattering, and pair production. It provides details on each mechanism, noting that the photoelectric effect dominates at low energies, pair production at very high energies above 1 MeV, and Compton scattering is predominant at medium energies. It also discusses absorption and transmission of photons in materials, how attenuation coefficients vary with photon energy and material properties like atomic number, and the spatial distribution of secondary radiation produced.
This article briefs on the commonly used different types of lasers, their working principle, applications, advantages and disadvantages. The types of lasers discussed in this section are
Nd-YAG Laser, Ruby Laser, Carbon Dioxide Laser, Semiconductor Laser, He-Ne Laser.
Lasers produce a very narrow, intense beam of coherent light through the process of stimulated emission of radiation. Key characteristics of laser light include high monochromaticity, directionality, intensity, and coherence. Einstein's theory of stimulated emission explains how excited atoms or molecules can emit photons when stimulated by an incoming photon, leading to amplification of the light beam. Population inversion, where more atoms are in an excited state than a lower state, must be achieved for lasing to occur. Common laser types include solid-state, gas, liquid/dye, and semiconductor lasers, which use different active media and pumping mechanisms to produce stimulated emission. A notable example is the Nd:YAG laser, which uses a neody
Solid State Electronics.
this slide is made from taking help of
TextBook
Ben.G.StreetmanandSanjayBanerjee:SolidStateElectronicDevices,Prentice-HallofIndiaPrivateLimited.
Nature and the characteristics of semi conductors(diodes and dopedWilson Jimmy
Group IV elements like silicon and germanium are semiconductors that have electrical conductivity between conductors and insulators. Their properties can be modified through doping, which involves adding small amounts of impurities. Doping silicon with elements having five valence electrons (like phosphorus) creates an n-type semiconductor with free electrons. Doping with elements having three valence electrons (like boron) creates a p-type semiconductor with holes. Placing a p-type and n-type semiconductor together forms a diode, which allows current to flow easily in only one direction.
1. A light emitting diode (LED) is a p-n junction diode that emits light when forward biased as electrons and holes recombine and release energy as photons.
2. The energy conversion in an LED occurs in two stages: carriers in the semiconductor absorb electrical energy raising them above equilibrium value, and most carriers give up this energy as spontaneous photon emission when they recombine.
3. The wavelength of light emitted by an LED depends on the bandgap of the semiconductor material, with lower bandgap materials emitting infrared light and higher bandgap materials emitting visible light.
The document summarizes key concepts in optics and optical properties of materials. It discusses topics like electromagnetic radiation spectrum, optical classifications of materials as transparent, translucent or opaque. It also covers concepts like reflection, refraction, absorption, transmission and how they relate to the band structure and band gaps of materials. Specific phenomena like fluorescence, phosphorescence, photoelasticity and their working principles are defined. Applications of optics like lasers, optical data storage are also briefly mentioned.
This document discusses the interactions between x-rays and matter. There are three main interactions - photoelectric effect, Compton scattering, and coherent scattering. The photoelectric effect occurs when a photon ejects an inner shell electron from an atom. This produces characteristic x-rays and leaves the atom ionized. Compton scattering involves the deflection of photons by outer shell electrons, producing scattered radiation. At diagnostic energies, Compton scattering is the most common interaction. The photoelectric effect dominates for high atomic number materials and low energy x-rays. These two interactions are most important in diagnostic radiology, while coherent scattering, pair production and photodisintegration occur at higher energies.
Basic of semiconductors and optical propertiesKamran Ansari
This presentation explains the band structure, intrinsic semiconductor, extrinsic semiconductor, electrical conductivity, mobility, hall effect, p-n junction diode, tunnel diode and optical properties of the semiconductor.
The document describes the operation of pn-junction and pin photodiodes. Pn-junction photodiodes convert light to electrical signals by separating electron-hole pairs generated by photon absorption in the depletion region. The quantum efficiency and responsivity characterize a photodiode's performance. Pin photodiodes have wider depletion widths than pn-junctions, allowing detection at higher frequencies and wavelengths. The intrinsic region in pin diodes provides a uniform electric field for carrier separation and drift, improving efficiency.
There are four main types of electrical polarization mechanisms: electronic, ionic, orientation, and space charge polarization. Electronic polarization occurs when an external electric field causes the nucleus and electron cloud of an atom to displace slightly, inducing a dipole moment. Ionic polarization is similar but occurs in ionic compounds due to displacement of ions from their equilibrium positions. Orientation polarization results from permanent molecular dipoles rotating to align with an applied field. Space charge polarization involves accumulation of charges at interfaces in dielectric materials when an electric field is applied. The total polarization of a material is generally the sum of these different polarization contributions.
1. The document discusses optical properties of semiconductors when exposed to electromagnetic radiation like light.
2. It explains concepts like absorption, reflection, transmission and emission spectra that can be obtained from materials and how they provide information about electronic band structures.
3. Key optical phenomena discussed include photon absorption promoting electrons from the valence to conduction band if the photon energy exceeds the semiconductor bandgap, and the interaction of light with materials leading to processes like reflection, refraction, scattering and dispersion.
X-rays can interact with matter through three main processes: the photoelectric effect, Compton effect, and pair production. The photoelectric effect occurs when an incoming photon ejects an inner shell electron. The ejected electron has kinetic energy and can ionize other atoms. The Compton effect happens when a photon collides with and ejects an outer shell electron. This produces a scattered photon and ejected electron. The probability of these interactions depends on factors like the photon energy and material's atomic number. High atomic number materials are stronger absorbers of x-rays via the photoelectric effect.
The document discusses the structure of atoms and the electromagnetic spectrum. It describes how atoms are made up of a nucleus surrounded by electrons in specific orbits. The electromagnetic spectrum is produced when charged particles accelerate and electromagnetic radiation travels as waves and particles. The different types of electromagnetic radiation are classified based on their wavelength, from long radio waves to short gamma rays.
The document discusses the mechanism behind photon emission in LEDs. It begins by explaining that in direct bandgap semiconductors, electron-hole recombination can directly produce photons without changing momentum. This allows efficient light emission. It then describes how different semiconductors like GaN, GaAsP, and GaP can be used to produce LEDs across the visible spectrum through modification of their bandgaps. The document concludes by discussing challenges in producing efficient blue LEDs and prospects for overcoming them.
1. LASER stands for 'Light Amplification by Stimulated Emission of Radiation'. It produces a very intense, concentrated, highly parallel and monochromatic beam of light.
2. Coherence is an important property of laser light. Ordinary light sources produce incoherent light with a wide range of frequencies, while laser produces coherent light that is uniform in frequency, amplitude, continuity and constant initial phase difference.
3. Population inversion is achieved by pumping atoms to a higher energy metastable state such that more atoms are in the excited state than the lower energy state. This allows for stimulated emission to overtake absorption, leading to amplification of light in the laser medium.
This document discusses semiconductor materials and devices. It begins by explaining electricity and electron bands in atoms. It then discusses the properties and atomic structures of conductors, insulators, and semiconductors. Semiconductors can be made to act as insulators or conductors through doping, which introduces impurity atoms. The document describes how n-type and p-type semiconductors are formed and their current flow. It concludes by explaining how a p-n junction diode is formed at the interface of p-type and n-type semiconductors and its current-voltage characteristics.
This document discusses semiconductor materials and their properties. It covers elemental and compound semiconductors, including gallium nitride used in LEDs. It describes the band structure of semiconductors including the valence and conduction bands separated by the bandgap. Carrier generation and recombination processes are explained. Intrinsic and extrinsic semiconductors are defined based on their carrier concentrations.
The document discusses the electro-optical properties of semiconductors under an applied electric field. It describes the Franz-Keldysh effect where an electric field causes a red shift and broadening of the band edge absorption in bulk semiconductors. It also discusses the Stark effect which modifies the excitonic absorption due to changes in the electron-hole interaction. When applied to quantum wells, the electric field can cause a quantum-confined Stark effect or quantum-confined Franz-Keldysh effect, broadening excitonic resonances and allowing forbidden transitions.
This document provides an overview of electrical properties of materials. It discusses how electrons move in different materials and the relationship between carrier density and mobility. Metals are good conductors due to their high number of free electrons. Semiconductors and insulators have lower conductivity since electrons must jump across a band gap. The document outlines band theory, explaining how energy bands arise from the interaction of atomic orbitals. Metals have partially filled or overlapping bands, allowing conduction, while semiconductors and insulators have filled valence bands separated from empty conduction bands by a band gap. Electrical properties depend on carrier concentration and mobility, with metals having high values of both.
Semiconductors have electrical properties between conductors and insulators. They behave as insulators at low temperatures but conduct electricity at room temperature due to their small band gap. Doping semiconductors with impurities creates an excess of electrons or holes, making them n-type or p-type. A p-n junction is formed at the boundary between p-type and n-type semiconductors and allows current to flow in only one direction, making it useful for diodes. Diodes are used to convert alternating current to direct current and have many applications in electronics.
Semiconductors have electrical properties between conductors and insulators. They conduct electricity better than insulators but not as well as metals. Semiconductors have small energy band gaps allowing electrons to move between valence and conduction bands with small amounts of energy. Semiconductors can be made intrinsic, with no impurities, or extrinsic through doping with elements from groups III/V. N-type doping adds free electrons while P-type adds holes. Intrinsic semiconductors have equal numbers of electrons and holes while extrinsic have more of one carrier type. Common semiconductors include silicon and germanium which have diamond cubic crystal structures.
Interaction of xrays and gamma rays with matter iiSneha George
The document discusses four main mechanisms by which photons interact with matter: coherent scattering, photoelectric effect, Compton scattering, and pair production. It provides details on each mechanism, noting that the photoelectric effect dominates at low energies, pair production at very high energies above 1 MeV, and Compton scattering is predominant at medium energies. It also discusses absorption and transmission of photons in materials, how attenuation coefficients vary with photon energy and material properties like atomic number, and the spatial distribution of secondary radiation produced.
This article briefs on the commonly used different types of lasers, their working principle, applications, advantages and disadvantages. The types of lasers discussed in this section are
Nd-YAG Laser, Ruby Laser, Carbon Dioxide Laser, Semiconductor Laser, He-Ne Laser.
Lasers produce a very narrow, intense beam of coherent light through the process of stimulated emission of radiation. Key characteristics of laser light include high monochromaticity, directionality, intensity, and coherence. Einstein's theory of stimulated emission explains how excited atoms or molecules can emit photons when stimulated by an incoming photon, leading to amplification of the light beam. Population inversion, where more atoms are in an excited state than a lower state, must be achieved for lasing to occur. Common laser types include solid-state, gas, liquid/dye, and semiconductor lasers, which use different active media and pumping mechanisms to produce stimulated emission. A notable example is the Nd:YAG laser, which uses a neody
LASER stands for Light Amplification by Stimulated Emission of Radiation. The first laser was constructed by Maiman. Lasers use stimulated emission to produce a coherent, collimated beam of light that is monochromatic, or consisting of a single wavelength. The key components of a laser are an active medium that can be excited to produce stimulated emission, and an optical cavity containing this medium bounded by mirrors forming a resonant cavity.
The document provides information on the basics of lasers and laser light. It defines LASER as an acronym for Light Amplification by Stimulated Emission of Radiation. It describes the key properties of laser beams including high coherence, intensity, directionality, and monochromaticity. It also discusses atomic transitions, population inversion, components of lasers including the active medium and optical resonator, and provides examples of specific lasers such as Nd:YAG lasers.
1. The document summarizes the components and operation of an argon ion laser. It describes the argon ion laser's active medium, pumping source using electrical discharge, and optical resonator.
2. Key components include a plasma tube with a beryllium oxide bore, mirrors to form an optical cavity, and a high voltage power supply. Population inversion is created when argon atoms are excited into higher energy levels via electron collisions.
3. Argon ion lasers emit multiple wavelengths between ultraviolet and green, including prominent lines at 488nm and 514.5nm. They have applications in spectroscopy, microscopy, surgery, and more.
This document discusses the basics of lasers, including their main components and properties. It explains that lasers work by inducing population inversion through pumping, allowing for stimulated emission to produce coherent, monochromatic beams of light. The key parts of a laser are its active medium, pumping source, and optical resonator. Examples of different laser types include solid state, gas, liquid/dye, and semiconductor lasers. Lasers have many applications in areas like communication, medicine, manufacturing, and research.
The document discusses lasers, including their characteristics and operation. It describes how lasers work via stimulated emission and population inversion. Nd:YAG lasers are discussed as a common solid-state laser type. Applications of lasers mentioned include medicine, manufacturing, communications, and more.
A He-Ne laser produces coherent red light through stimulated emission. It works by electrically exciting a gas mixture of helium and neon atoms. Energy from excited helium atoms is transferred to neon atoms, producing population inversion between neon energy levels. When excited neon atoms drop to a lower energy level, they emit photons of 632.8 nm wavelength that stimulate additional photon emissions, producing a coherent laser beam. He-Ne lasers operate continuously and are commonly used for applications like barcode scanning and holography due to their low cost and narrow visible beam.
This document provides an overview of different types of lasers and their applications. It discusses solid state lasers like ruby lasers, gaseous lasers like He-Ne lasers, and semiconductor lasers like Ga-As lasers. For each laser, it describes the active medium, construction, pumping mechanism, working principle, and some applications. Ruby lasers were historically used for applications like holography and tattoo removal. He-Ne lasers emit red light at 632nm and are used in applications like bar code scanners and holography. Semiconductor lasers like Ga-As lasers are compact, efficient sources used in devices like DVD players, fiber optic networks, and laser printers.
The document discusses the helium-neon (He-Ne) laser, which was the first continuous laser invented by Javan et al. in 1961. It operates at a wavelength of 632.8 nm in the red portion of the visible spectrum. The He-Ne laser consists of a glass tube containing a mixture of helium and neon gases that is excited by an electrical discharge. When an excited helium atom collides with a neon atom, the neon atom becomes excited and subsequently decays, emitting a photon that stimulates further photon emissions to generate the laser beam. He-Ne lasers have various applications including reading barcodes and producing holograms.
The document discusses the construction and operation of a laser diode. It describes how a laser diode is made of two gallium arsenide layers that form a p-n junction. When a voltage is applied, electrons are excited across the junction, causing spontaneous emission of photons. These photons stimulate additional electrons to emit more photons through stimulated emission, producing a coherent beam of light that exits through the partially reflective end of the diode. Laser diodes have advantages like low cost, small size, and high reliability, and they are used in applications such as fiber optics, barcode readers, and laser printing.
Communication Engineering LED and LASER Sources.pptMdYekraRahman1
This document summarizes key concepts about optical sources used in fiber optic communications. It discusses two main types of optical sources - light emitting diodes (LEDs) which produce incoherent light, and lasers which produce coherent light via stimulated emission. Lasers require population inversion and optical feedback to produce amplification of light. Semiconductor lasers use materials like gallium arsenide to produce population inversion through injection of electrons and holes across a p-n junction. Heterojunction lasers confine light and carriers better for lower lasing thresholds.
The document provides an overview of lasers, including their introduction, characteristics, population inversion, types of coherence, and applications. It discusses key laser concepts such as spontaneous emission, stimulated emission, optical pumping, threshold inversion density, and optical feedback. Examples of specific laser types are given, including ruby lasers, HeNe lasers, and semiconductor lasers. The document concludes with applications of lasers in areas like welding, medicine, data storage, printing, and military weapons.
Principle And Working of A Semiconductor Laser.pptxRehmanRasheed3
The document summarizes the principles and working of a semiconductor laser, explaining that it uses stimulated emission from a p-n junction diode made of gallium arsenide to produce coherent infrared laser light, and that applying a forward voltage bias injects electrons and holes to achieve population inversion and trigger stimulated recombination of photons within the diode's optical resonator structure. Semiconductor lasers have applications in fiber optic communication, wound healing, laser printing, and CD/DVD reading/writing due to their compact size, high efficiency, and ability to produce continuous or pulsed laser output.
1) The document describes the helium-neon laser, which was invented in 1960 and works on the principle of a four-level laser system.
2) It consists of a glass tube containing a mixture of helium and neon gases, along with electrodes that provide an electric discharge to excite the gases.
3) When excited by the discharge, helium atoms transfer their energy to neon atoms, pushing them into metastable energy levels. Stimulated emission then occurs as the neon atoms fall from these levels, producing the laser beam.
The document provides an overview of lasers, including:
1) It defines what a laser is and describes the three main processes that occur in lasers: absorption, spontaneous emission, and stimulated emission.
2) It explains the key components of lasers - the active medium, pumping mechanism, and optical resonator.
3) It provides examples of different types of lasers, including ruby, He-Ne, and semiconductor lasers, and describes their workings.
4) It discusses applications of lasers in various fields such as industry, medicine, communications, defense, and more.
The document discusses different types of gas lasers, including helium-neon (He-Ne) lasers, carbon dioxide lasers, nitrogen lasers, and argon lasers. It provides details on the construction, working principle, and applications of each laser. The He-Ne laser was the first continuous laser invented in 1961. It operates at 632.8 nm in the red spectrum and is often used for demonstrations and reading barcodes. Carbon dioxide lasers produce a high-power infrared beam and are commonly used for industrial cutting and welding. Nitrogen lasers emit ultraviolet light in short pulses. Argon lasers can output multiple wavelengths ranging from ultraviolet to green.
This document provides information about lasers and optical fibers. It begins with definitions of lasers and describes the characteristics of laser light such as monochromaticity, directionality, coherence and brightness. It then discusses population inversion and the basic requirements for a laser system including the pumping system, active medium and optical resonator. Specific laser types are described like ruby lasers, He-Ne lasers and semiconductor lasers. Optical fibers are also summarized, including their construction, principles of total internal reflection, acceptance angle, numerical aperture and types such as step-index and graded-index fibers.
The document describes the helium-neon laser. It discusses how the laser works through a four-level process involving helium and neon gases. First, a helium atom is excited through electron collision and transfers its energy to a neon atom, creating population inversion. Then, as excited neon atoms decay to a lower energy level, they emit 632nm photons through stimulated emission, producing the laser beam. Finally, the neon atoms decay further through spontaneous emission or collision with the tube wall. Applications include barcode scanners, holography, and laboratory demonstrations due to the laser's narrow red beam.
it describes the bony anatomy including the femoral head , acetabulum, labrum . also discusses the capsule , ligaments . muscle that act on the hip joint and the range of motion are outlined. factors affecting hip joint stability and weight transmission through the joint are summarized.
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A review of the growth of the Israel Genealogy Research Association Database Collection for the last 12 months. Our collection is now passed the 3 million mark and still growing. See which archives have contributed the most. See the different types of records we have, and which years have had records added. You can also see what we have for the future.
Assessment and Planning in Educational technology.pptxKavitha Krishnan
In an education system, it is understood that assessment is only for the students, but on the other hand, the Assessment of teachers is also an important aspect of the education system that ensures teachers are providing high-quality instruction to students. The assessment process can be used to provide feedback and support for professional development, to inform decisions about teacher retention or promotion, or to evaluate teacher effectiveness for accountability purposes.
How to Manage Your Lost Opportunities in Odoo 17 CRMCeline George
Odoo 17 CRM allows us to track why we lose sales opportunities with "Lost Reasons." This helps analyze our sales process and identify areas for improvement. Here's how to configure lost reasons in Odoo 17 CRM
This presentation includes basic of PCOS their pathology and treatment and also Ayurveda correlation of PCOS and Ayurvedic line of treatment mentioned in classics.
A Strategic Approach: GenAI in EducationPeter Windle
Artificial Intelligence (AI) technologies such as Generative AI, Image Generators and Large Language Models have had a dramatic impact on teaching, learning and assessment over the past 18 months. The most immediate threat AI posed was to Academic Integrity with Higher Education Institutes (HEIs) focusing their efforts on combating the use of GenAI in assessment. Guidelines were developed for staff and students, policies put in place too. Innovative educators have forged paths in the use of Generative AI for teaching, learning and assessments leading to pockets of transformation springing up across HEIs, often with little or no top-down guidance, support or direction.
This Gasta posits a strategic approach to integrating AI into HEIs to prepare staff, students and the curriculum for an evolving world and workplace. We will highlight the advantages of working with these technologies beyond the realm of teaching, learning and assessment by considering prompt engineering skills, industry impact, curriculum changes, and the need for staff upskilling. In contrast, not engaging strategically with Generative AI poses risks, including falling behind peers, missed opportunities and failing to ensure our graduates remain employable. The rapid evolution of AI technologies necessitates a proactive and strategic approach if we are to remain relevant.
This slide is special for master students (MIBS & MIFB) in UUM. Also useful for readers who are interested in the topic of contemporary Islamic banking.
Thinking of getting a dog? Be aware that breeds like Pit Bulls, Rottweilers, and German Shepherds can be loyal and dangerous. Proper training and socialization are crucial to preventing aggressive behaviors. Ensure safety by understanding their needs and always supervising interactions. Stay safe, and enjoy your furry friends!
ISO/IEC 27001, ISO/IEC 42001, and GDPR: Best Practices for Implementation and...PECB
Denis is a dynamic and results-driven Chief Information Officer (CIO) with a distinguished career spanning information systems analysis and technical project management. With a proven track record of spearheading the design and delivery of cutting-edge Information Management solutions, he has consistently elevated business operations, streamlined reporting functions, and maximized process efficiency.
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What sets Denis apart is his comprehensive understanding of Business and Systems Analysis technologies, honed through involvement in all phases of the Software Development Lifecycle (SDLC). From meticulous requirements gathering to precise analysis, innovative design, rigorous development, thorough testing, and successful implementation, he has consistently delivered exceptional results.
Throughout his career, he has taken on multifaceted roles, from leading technical project management teams to owning solutions that drive operational excellence. His conscientious and proactive approach is unwavering, whether he is working independently or collaboratively within a team. His ability to connect with colleagues on a personal level underscores his commitment to fostering a harmonious and productive workplace environment.
Date: May 29, 2024
Tags: Information Security, ISO/IEC 27001, ISO/IEC 42001, Artificial Intelligence, GDPR
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3. He-Ne LASER
He-Ne stands for Helium-Neon, Was the first continuous laser.
In this laser active medium consists of mixture of helium and neon gases which do not interact, so
one type of atomic gas lasers
He-Ne gases are taken in 10:1 ratio
Electric discharge is used as pumping source
It is a four level laser
Its usual operation wavelength is 632.8 nm, in the red portion of the visible spectrum.
17 April 2019 3
4. CONSTRUCTION
The setup consists of a discharge tube of length 80 cm and bore diameter of 1.0 cm.
Mixture of helium and neon gases maintained at low pressure (an average 50 Pa per cm of cavity
length ) in a glass envelope.
consists of a glass envelop with a narrow capillary tube through the center. The capillary tube is
designed to direct the electrical discharge through its small bore to produce very high current
densities in the gas.
The plasma tube has a large cylindrical metallic cathode and a smaller metallic anode. The current is
directed from cathode to anode.
The energy or pump source of the laser is provided by an electrical discharge of around 1000 volts
through an anode and cathode at each end of the glass tube. A current of 5 to 100 mA is typical for
CW operation.
The optical cavity of the laser typically consists of a plane, high reflecting mirror at one end of the
laser tube, and a concave output coupler mirror of approximately 1% transmission at the other end.
He-Ne lasers are normally small, with an optical output powers ranging from 1 mW to 100 mW.
Output power of these lasers depends on the length of the discharge tube and pressure of the gas
mixture17 April 2019 4
6. WORKING
In the He-Ne laser the light is produced by atomic transitions within the Neon atom.
The Helium does not directly produce laser light but it acts as a buffer gas, the purpose of which is
to assist/help the atoms of the other gas to produce lasing in as manner.
When energy from the pumping source is applied (voltage applied) in He-Ne gas mixture then some
of the energy is observed by the Helium atoms.ie, the helium atoms achieve an excited state.
Now when the Helium atoms move within the laser tube, they collide with the Neon atoms. At each
collision some of the energy within the helium atom is transferred to the Neon atom and so raising
it to an excited meta-stable state.
When a sufficient number of Neon atoms reach to this state then population inversion occurs and
hence the lasing can take place.
17 April 2019 6
8. On collision with fast moving electrons He atoms get excited to F2
and F3 energy levels, where
lifetime of helium atoms is more. So maximum possibility of energy transfer between He and Ne
atoms through atomic collisions.
Thus Ne atoms get excited to E4 and E6, continuous excitation attains population inversion.
Transitions from E6 to E5 and E4 to E3 corresponds to infrared region
Transition from E6 to E3 corresponds to visible region, Red colour in visible spectrum.
Ne atoms present in E3 level are de-excited to E2 level by spontaneous emission and from there on
colliding with walls of the tube gets de-excited to ground level E1
17 April 2019 8
9. INJECTION LASER
An injection laser, also known as an laser diode or diode laser
It is a specially fabricated PN junction device, which emits coherent light when forward biased
The basic mechanism responsible for light emission from a semiconductor is the recombination of electrons and holes at a p-n
junction when a current is passed through a diode
Conversion of electrical energy to light energy
The material which often used in Laser diode is the gallium Arsenide (GaAs) in (homojunction)
In order to design a laser diode, the p-n junction must be heavily doped (degenerately doped).
Population inversion is required for producing stimulated emission. A P-N diode consist of electrons and holes distributed in
respective energy bands. Therefore laser action in this type of diode involves energy bands rather than discrete levels
Unlike in other lasers population inversion is not obtained by exciting electrons in spatially isolated atoms but injecting into the
conduction band from the external circuit, thus the name injection laser
Thus attaining a condition of large concentration of electrons in the conduction band and a large concentration of holes in the
valence band.
Therefore the conduction band plays the role of excited level while the valence band plays the role of ground level.17 April 2019 9
10. CONSTRUCTION
Consist of a heavily doped PN junction, starting with a heavily
doped N type GaAs material and a heavily zinc doped layer
constitutes the heavily doped P region formed on its top.
By doping, the Fermi level of the n-side will lie in the
conduction band whereas the Fermi level in the p-region will lie
in the valance band.
The top and bottom surfaces are provided with metal contacts
(metallized) to pass current through the diode
The front and rear faces are polished parallel to each other and
perpendicular to the plane of the junction
The remaining two sides of the diode are roughened to
eliminate lasing action in that direction
17 April 2019 10
11. WORKING
When PN junction is forward biased, electron and holes are injected into the junction region (active region) in high
concentrations. at low forward current the electron hole recombination causes spontaneous emission of photons and
the junction acts as an LED.
On increasing the forward current the intensity of the light increases linearly and when it reaches the threshold value,
the carrier concentration in the junction region will rise to a very high value as a result junction region contains a large
concentration of electrons within the conduction band and simultaneously a large number of holes within valence band
(holes represent absence of electron)
Thus the upper energy level in the narrow region are having a high electron population while the lower energy levels in
the same region are vacant (holes), the condition of population inversion attained in active region or depletion region or
inversion region
Recombination acts of electron and hole pairs lead to spontaneous emission of photons which propagating in the
junction plane stimulate the conduction electron to jump into vacant states of valence band
This stimulated electron hole recombination produces coherent radiation, GaAs laser emits at a wavelength of 9000Å
17 April 2019 11
13. Nd-YAG LASER
Neodymium-doped Yttrium Aluminum Garnet ( Y3Al5O12), Nd: YAG laser is a solid state laser in which
Nd: YAG is used as a laser medium.
Nd: YAG laser is a four-level laser system, which means that the four energy levels are involved in
laser action. These lasers operate in both pulsed and continuous mode.
Nd: YAG laser generates laser light commonly in the near-infrared region of the spectrum at 1064
nanometers (nm). It also emits laser light at several different wavelengths including 1440 nm, 1320
nm, 1120 nm, and 940 nm
In Nd: YAG laser, light energy sources such as flashtube are used as energy source to supply energy
to the active medium.
17 April 2019 13
14. CONSTRUCTION
Energy source
The energy source or pump source supplies energy to the active medium to achieve population
inversion. In Nd: YAG laser, light energy sources such as flashtube or laser diodes are used as energy
source to supply energy to the active medium.
17 April 2019 14
15. Active medium
The active medium or laser medium of the Nd:YAG laser is made up of a synthetic crystalline material
(Yttrium Aluminum Garnet (YAG)) doped with a chemical element (neodymium (Nd)). The lower energy
state electrons of the neodymium ions are excited to the higher energy state to provide lasing action in
the active medium.
Nd3+ ions act as active medium or active centres. YAG is just the host.
Optical resonator
The Nd:YAG crystal is placed between two mirrors. These two mirrors are optically coated or silvered.
Each mirror is silvered or coated differently. One mirror is fully silvered whereas, another mirror is partially
silvered. The mirror, which is fully silvered, will completely reflect the light and is known as fully reflecting
mirror.
On the other hand, the mirror which is partially silvered will reflect most part of the light but allows a
small portion of light through it to produce the laser beam. This mirror is known as a partially reflecting
mirror
17 April 2019 15
16. WORKING
Nd: YAG laser is a four-level laser system, which means that the four energy levels are involved in laser
action.
In Nd:YAG laser, the lower energy state electrons in the neodymium ions are excited to the higher energy
state to achieve population inversion.
Consider a Nd:YAG crystal active medium consisting of four energy levels E1, E2, E3, and E4.
The energy levels will be E1 < E2 <E3 <E4. The energy level E1 is known as ground state, E2 is the next
higher energy state or excited state, E3 is the metastable state and E4 is the excited state.
When flashtube or laser diode supplies light energy to the active medium (Nd:YAG crystal), the lower
energy state (E1) electrons in the neodymium ions gets excited to the higher energy state E4.
The lifetime of higher energy state E4 is very small (230 microseconds) so the electrons in the energy
state E4 do not stay for long period. After a short period, the electrons will fall into the next lower energy
state or metastable state E3 by releasing non-radiation energy (releasing energy without emitting
photons).
The lifetime of metastable state E3 is high compared to E4. This results in an increase in the number of
electrons in the metastable E3 and hence population inversion is achieved.
17 April 2019 16
17. After some period, the electrons in the metastable state E3 will fall into the next lower energy state
E2 by releasing photons or light. The emission of photons in this manner is called spontaneous
emission.
The lifetime of energy state E2 is very small just like the energy state E4. Therefore, after a short
period, the electrons in the energy state E2 will fall back to the ground state E1 by releasing radiation
less energy.
When photon emitted due to spontaneous emission is interacted with the other metastable state
electron, it stimulates that electron and makes it fall into the lower energy state by releasing the
photon. As a result, two photons are released. The emission of photons in this manner is called
stimulated emission of radiation.
Spontaneous emission is a natural process but stimulated emission is not a natural process. To
achieve stimulated emission, we need to supply external photons or light to the active medium.
The Nd:YAG active medium generates photons or light due to spontaneous emission. The light or
photons generated in the active medium will bounce back and forth between the two mirrors. This
stimulates other electrons to fall into the lower energy state by releasing photons or light. Likewise,
millions of electrons are stimulated to emit photons.
The light generated within the active medium is reflected many times between the mirrors before it
escapes through the partially reflecting mirror
17 April 2019 17
19. DYE LASER
• A dye laser is a laser which uses an organic dye as the lasing medium, usually a liquid solution.
• A dye is a coloured substance which imparts its colour to the material it is being applied
• Active medium for the dye laser is the organic dye
• Some of the organic dyes are Rhodamine 6G, Fluorescein, coumarin
• Flash lamps and several types of lasers can be used to optically pump dye lasers
• The main advantage of this type of laser is its tunability, which means lasing wavelength for a dye
may be varied over wide range,
• so it is also called as tunable lasers
• Tuning over 500 angstrom has been obtained.
17 April 2019 19
20. CONSTRUCTION
Dye laser consisted of a 1cm long quartz glass tube filled with solutions of organic dyes
Organic dyes are dissolved in solvents like water, ethyl alcohol, methanol.
Active medium = organic dye + water, benzene, ethanol
The dye solution typically has a concentration in the range of 10-2 to 10-4 M
Energy for optical pumping is provided by flash lamp
Tuning can be obtained by replacing one of the mirrors of the resonant cavity with a diffraction
grating.
By rotating the diffraction grating wavelength of the laser output can be altered.
17 April 2019 20
22. WORKING & ENERGY DIAGRAM
The main difference is the use of dye as active medium which is dissolved in suitable solvent.
Absorption from S0 to S1, S2
Rapid collisional relaxation to ground vibrational level of S1
Fluorescence to various vibrational states of S0 (basis for laser
emission)
ISC (inter system crossing) to state T1
pumping at 1 or 2; laser emission at 5
If flash lamp is used for optical pumping output is pulsed laser
If other laser sources are used for optical pumping output is
continuous wave laser
17 April 2019 22