Laser in physics

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ACTIVE LEARNING ASSIGNMENT TOPIC:LASER

Transcript of Laser in physics

Page 1: Laser in physics

ACTIVE LEARNING ASSIGNMENT

TOPIC:LASER

Page 2: Laser in physics

Physics (2110011)

Branch-1st sem ITDiv-DBatch-D1

Guided by:- prof. Nirav PandyaPrepaid by:-(1) Gelani Ravikumar A.(2) Chovatiya Jay M.(3) Dabhi Jayraj M.

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Introduction on LASER

› LASER is a acronym for Light Amplification by Stimulated Emission of Radiation. In Laser the intensity of light is amplified by a process called stimulated emission.

› The laser is perhaps the most important optical device to be developed in the past 50 years. Since its arrival in the 1960s, rather quiet and unheralded outside the scientific community, it has provided the stimulus to make optics one of the most rapidly growing fields in science and technology today.

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› In 1960, T.H.Maiman built the first laser device (ruby laser). Within months of the arrival of Maiman’s ruby laser, which emitted deep red light at a wavelength of 694.3 nm, A. Javan and associates developed the first gas laser (He-Ne laser), which emitted light in both the infrared (at 1.15mm) and visible

(at 632.8 nm) spectral regions.

› Following the birth of the ruby and He-Ne lasers, others devices followed in rapid succession, each with a different laser medium and a different wavelength emission. For the greater part of the 1960s, the laser was viewed by the world of industry and technology as scientific curiosity.

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Principle of laser

It is based on the principle of stimulated emission of radiation, with light amplification. For stimulated emission of radiation to take place, the population of atoms in higher energy level should be greater than the lower energy level, i.e., N2>N1 . This can be achieved by pumping. Light amplification is achieved by photon multiplication within an optical resonator cavity.

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Characteristics of LASERThe following characteristics, distinguishes a laser beam from an ordinary light.

› Coherence: The wave trains which are identical in phase and direction are called coherent waves.

› High intensity: Due to the coherent nature of laser, it has ability to focus over a small area of 10-6 cm2.

› High directionality: an ordinary light source emits light in all possible directions. But, laser travels as a parallel beam it can travel over a long distance without spreading.

› Monochromaticity: The light from a normal monochromatic source spreads over a range of wavelength of the order 100nm. But, the spread is of 1nm for laser.

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Einstein’s quantum theory of radiation

In 1916, according to Einstein, the interaction of radiation with matter could be explained in terms of three basic processes:

1. Induced absorption.2. Spontaneous Emission.3. Stimulated Emission.

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Spontaneous EmissionIt is a process in which there is an emission of a photon whenever an atom transmits from a higher energy state to a lower energy state without the aid of any external agency.

For this process to take place, the atom has to be in the excited state. Since, the higher energy level is an unstable one, the excited atom in the higher level E2 spontaneously returns to the lower energy level E1 with the emission of a photon of a energy hv=E2-E1.

Atom* Atom + Photon

The rate of spontaneous emission of radiation R21 (sp) is proportional to the population N2 at the higher energy level E2.

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Stimulated Emission

It is a process in which there is an emission of a photon whenever an atom transits from a higher energy level to a lower energy level under the influence of a external agency, i.e., an inducing photon.

For this process also, the atom should be already in the excited state. Let a photon having an energy hv=E2-E1 interact with an atom in the excited state. Under such interaction, the incident photon stimulate the excited atom in the level E2 to transit to the lower energy level E1, resulting in the emission of a photon of energy hv=E2-E1.

Atom +Photon

Atom(Photon + Photon)

The rate of stimulated emission of radiation R21(st) is proportional to the population N2 at the higher energy level E2 and to the density ρof the including photon.

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Population Inversion

Population inversion is a state of a achieving more number of atoms in the excited state compared to the ground state.

i.e., N2 > N1

If the condition is satisfied, then there is more chance for stimulated emission to take place. Hence, population inversion is an essential condition for producing laser.

Population inversion can be achieved by a process called pumping.

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PumpingPumping is the mechanism of exciting atoms from lower energy state to a higher energy state by supplying energy from an external source. The most commonly used pumping mechanism are,

› Optical pumping: In this type of pumping atoms are excited by means of an external optical source.

eg: Ruby LASER and Nd:YAG LASER.

› Electrical pumping: In this type of pumping the electrons are accelerated to a high velocity by a strong electric field. These moving electrons collide with the neutral gas and ionize the medium. Thus, due to ionization they get raised to a higher energy level.

eg: CO2 LASER.

› Direct conversion: In this type of pumping a direct conversion of electric energy into light takes place.

eg: Semiconductor LASER.

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Applications of LASER

a)In Industry (1) For welding and melting. (2) For cutting and drilling holes. (3) To test the quality of the materials.

b)In Medicine(1) Used for the treatment of detached retinas.(2) Used in performing micro and bloodless surgery.(3) used for the treatment of human and animal

cancers and skin tumors.

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c)Military applications(1) The laser beam can serve as a war weapon.(2) The laser beam can be used to determine

precisely the distance, velocity and direction from a distant objects by means of the reflected signal.

d)Science and engineering applications(1) It is used in fiber optic communication.(2) It is used in holography.(3) It is used in underwater communication between

submarines

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