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ND:YAG LASER
PREPARED BY :~
DHRUPAL S PATEL
ND: YAG LASER (DOPED INSULATOR LASER) :
LASING MEDIUM :
 THE HOST MEDIUM FOR THIS LASER IS YTTRIUM
ALUMINIUM GARNET (YAG = Y3 AL5 O12) WITH 1.5%
TRIVALENT NEODYMIUM IONS (ND3+) PRESENT AS
IMPURITIES.
 THE (ND3+) IONS OCCUPY THE LATTICE SITES OF
YTTRIUM IONS AS SUBSTITUTIONAL IMPURITIES
AND PROVIDE THE ENERGY LEVELS FOR BOTH
PUMPING AND LASING TRANSITIONS.
 WHEN AN (ND3+) ION IS PLACED IN A HOST
CRYSTAL LATTICE IT IS SUBJECTED TO THE
ELECTROSTATIC FIELD OF THE SURROUNDING
IONS, THE SO CALLED CRYSTAL FIELD.
 THE CRYSTAL FIELD MODIFIES THE TRANSITION
PROBABILITIES BETWEEN THE VARIOUS ENERGY
LEVELS OF THE ND3+ ION SO THAT SOME
TRANSITIONS, WHICH ARE FORBIDDEN IN THE
FREE ION, BECOME ALLOWED
 THE LENGTH OF THE ND: YAG LASER ROD
VARIOUS FROM 5CM TO 10CM DEPENDING ON
THE POWER OF THE LASER AND ITS DIAMETER
IS GENERALLY 6 TO 9 MM.
 THE LASER ROD AND A LINEAR FLASH LAMP
ARE HOUSED IN A ELLIPTICAL REFLECTOR
CAVITY
 SINCE THE ROD AND THE LAMP ARE LOCATED
AT THE FOCI OF THE ELLIPSE, THE LIGHT
EMITTED BY THE LAMP IS EFFECTIVELY
COUPLED TO THE ROD.
 THE ENDS OF THE ROD ARE POLISHED AND
MADE OPTICALLY FLAT AND PARALLEL.
 THE OPTICAL CAVITY IS FORMED EITHER BY
SILVERING THE TWO ENDS OF THE ROD OR BY
USING TWO EXTERNAL REFLECTING MIRRORS.
 ONE MIRROR IS MADE HUNDRED PERCENT
REFLECTING WHILE THE OTHER MIRROR IS
LEFT SLIGHTLY TRANSMITTING TO DRAW THE
OUTPUT
 THE SYSTEM IS COOLED BY EITHER AIR OR
WATER CIRCULATION
 THIS LASER SYSTEM HAS TWO ABSORPTION
BANDS (0.73 M AND 0.8 M)
 OPTICAL PUMPING MECHANISM IS
EMPLOYED.
 LASER TRANSITION TAKES PLACE BETWEEN
TWO LASER LEVELS AT 1.06 MM.
OUTPUT CHARACTERISTICS :
 THE LASER OUTPUT IS IN THE FORM OF PULSES
WITH HIGHER REPETITION RATE
 XENON FLASH LAMPS ARE USED FOR PULSED
OUTPUT.
 ND: YAG LASER CAN BE OPERATED IN CW MODE
ALSO USING TUNGSTEN-HALIDE INCANDESCENT
LAMP FOR OPTICAL PUMPING.
 CONTINUOUS OUTPUT POWERS OF OVER 1KW
ARE OBTAINED.
NOTE: ND: GLASS LASER :
 GLASS ACTS AS AN EXCELLENT HOST MATERIAL FOR
NEODYMIUM.
 AS IN YAG, WITHIN THE GLASS ALSO LOCAL ELECTRIC
FIELDS MODIFY THE ND3+ ION ENERGY LEVELS.
 SINCE THE LINE WIDTH IS MUCH BROADER IN GLASS
THAN IN YAG FOR ND3+ IONS, THE THRESHOLD PUMP
POWER REQUIRED FOR LASER ACTION IS HIGHER.
 ND: GLASS LASERS ARE OPERATED IN THE PULSED MODE
AT WAVELENGTH 1.06 M
Nd:YAG/ Nd: Glass laser applications :
 These lasers are used in many scientific applications
which involve generation of other wavelengths of light.
 The important industrial uses of YAG and glass lasers
have been in materials processing such as welding,
cutting, drilling.
 Since 1.06 m wavelength radiation passes through
optical fibre without absorption, fibre optic endoscopes
with YAG lasers are used to treat gastrointestinal
bleeding.
 YAG lasers are used in military as range finders
and target designators.
 YAG beams penetrate the lens of the eye to
perform intracular procedures

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ND YAG laser

  • 1. ND:YAG LASER PREPARED BY :~ DHRUPAL S PATEL
  • 2. ND: YAG LASER (DOPED INSULATOR LASER) : LASING MEDIUM :  THE HOST MEDIUM FOR THIS LASER IS YTTRIUM ALUMINIUM GARNET (YAG = Y3 AL5 O12) WITH 1.5% TRIVALENT NEODYMIUM IONS (ND3+) PRESENT AS IMPURITIES.  THE (ND3+) IONS OCCUPY THE LATTICE SITES OF YTTRIUM IONS AS SUBSTITUTIONAL IMPURITIES AND PROVIDE THE ENERGY LEVELS FOR BOTH PUMPING AND LASING TRANSITIONS.
  • 3.  WHEN AN (ND3+) ION IS PLACED IN A HOST CRYSTAL LATTICE IT IS SUBJECTED TO THE ELECTROSTATIC FIELD OF THE SURROUNDING IONS, THE SO CALLED CRYSTAL FIELD.  THE CRYSTAL FIELD MODIFIES THE TRANSITION PROBABILITIES BETWEEN THE VARIOUS ENERGY LEVELS OF THE ND3+ ION SO THAT SOME TRANSITIONS, WHICH ARE FORBIDDEN IN THE FREE ION, BECOME ALLOWED
  • 4.
  • 5.  THE LENGTH OF THE ND: YAG LASER ROD VARIOUS FROM 5CM TO 10CM DEPENDING ON THE POWER OF THE LASER AND ITS DIAMETER IS GENERALLY 6 TO 9 MM.  THE LASER ROD AND A LINEAR FLASH LAMP ARE HOUSED IN A ELLIPTICAL REFLECTOR CAVITY  SINCE THE ROD AND THE LAMP ARE LOCATED AT THE FOCI OF THE ELLIPSE, THE LIGHT EMITTED BY THE LAMP IS EFFECTIVELY COUPLED TO THE ROD.  THE ENDS OF THE ROD ARE POLISHED AND MADE OPTICALLY FLAT AND PARALLEL.
  • 6.  THE OPTICAL CAVITY IS FORMED EITHER BY SILVERING THE TWO ENDS OF THE ROD OR BY USING TWO EXTERNAL REFLECTING MIRRORS.  ONE MIRROR IS MADE HUNDRED PERCENT REFLECTING WHILE THE OTHER MIRROR IS LEFT SLIGHTLY TRANSMITTING TO DRAW THE OUTPUT  THE SYSTEM IS COOLED BY EITHER AIR OR WATER CIRCULATION
  • 7.  THIS LASER SYSTEM HAS TWO ABSORPTION BANDS (0.73 M AND 0.8 M)  OPTICAL PUMPING MECHANISM IS EMPLOYED.  LASER TRANSITION TAKES PLACE BETWEEN TWO LASER LEVELS AT 1.06 MM.
  • 8. OUTPUT CHARACTERISTICS :  THE LASER OUTPUT IS IN THE FORM OF PULSES WITH HIGHER REPETITION RATE  XENON FLASH LAMPS ARE USED FOR PULSED OUTPUT.  ND: YAG LASER CAN BE OPERATED IN CW MODE ALSO USING TUNGSTEN-HALIDE INCANDESCENT LAMP FOR OPTICAL PUMPING.  CONTINUOUS OUTPUT POWERS OF OVER 1KW ARE OBTAINED.
  • 9. NOTE: ND: GLASS LASER :  GLASS ACTS AS AN EXCELLENT HOST MATERIAL FOR NEODYMIUM.  AS IN YAG, WITHIN THE GLASS ALSO LOCAL ELECTRIC FIELDS MODIFY THE ND3+ ION ENERGY LEVELS.  SINCE THE LINE WIDTH IS MUCH BROADER IN GLASS THAN IN YAG FOR ND3+ IONS, THE THRESHOLD PUMP POWER REQUIRED FOR LASER ACTION IS HIGHER.  ND: GLASS LASERS ARE OPERATED IN THE PULSED MODE AT WAVELENGTH 1.06 M
  • 10. Nd:YAG/ Nd: Glass laser applications :  These lasers are used in many scientific applications which involve generation of other wavelengths of light.  The important industrial uses of YAG and glass lasers have been in materials processing such as welding, cutting, drilling.  Since 1.06 m wavelength radiation passes through optical fibre without absorption, fibre optic endoscopes with YAG lasers are used to treat gastrointestinal bleeding.
  • 11.  YAG lasers are used in military as range finders and target designators.  YAG beams penetrate the lens of the eye to perform intracular procedures