2. INTRODUCTION
o Lasers: A highly useful source in analytical
instrumentation
high intensities
narrow band widths
coherent nature of their outputs
o Laser
Light Amplification by Stimulated Emission of
Radiation.
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3. COMPONENTS OF LASER
Mainly three components:
Lasing medium:
a solid crystal such as ruby, a semiconductor
such as gallium arsenide, a solution of an organic
dye, or a gas such as argon or krypton is used.
Energy pump source:
The lasing material is activated by radiation from
an external source.
A few photons of proper energy will trigger
formation of a cascade of photons of same
energy.
Resonator cavity:
causes enormous amplification of photons 3
6. PUMPING
Necessary for laser action.
When an electric current is passed or
exposure to an intense radiant source, active
species of laser get excited by means of an
electrical discharge.
During pumping several higher electronic
and vibrational energy levels are produced.
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8. SPONTANEOUS EMISSION
Same as in case of fluorescence.
Species in an excited electronic state may
lose whole or a part of its excess energy
by spontaneous emission of radiation.
wavelength of radiation is given by
λ= hc /Ey-Ex
h- Plank’s constant
c- speed of light
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10. STIMULATED EMISSION
In this excited laser species are struck by
photons that have precisely the same
energies Ey-Ex as the photons produced
by the spontaneous emission.
This collision may cause the excited
species to relax immediately to lower
energy level & thus emits a photon of
same energy as that of the photon that
stimulated the process.
Stimulated emission is coherent with the
incoming radiations.
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12. ABSORPTION
The absorption process which completes
with stimulated emission.
Here 2 photons with energies exactly
equal to (Ey-Ex) are absorbed to produce
the Metastable excited state
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14. POPULATION INVERSION & LIGHT
AMPLIFICATION
For light amplification in a laser, it is
necessary that the number of photos
produced by stimulated emission exceed the
number lost by absorption.
Therefore, number of particles in the higher
energy state exceeds the number in the
lower.
In other words, there must be a population
inversion
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16. THREE & FOUR LEVEL SYSTEMS
Three level:
transition between excited state Ey and the
ground state Eo.
Four level:
transition between excited state Ey and the Ex
state. Ex has greater energy than Eo.
Population inversion is readily achieved in
four-level system.
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18. TYPES OF LASERS
Gas lasers
Dye lasers
Solid state lasers
Semiconductor lasers
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19. Gas Lasers
Gas lasers are typically excited by an
electrical discharge.
Four types:-
Neutral atom lasers: He/Ne(632.8nm)
Ion lasers in which active species is Ar+ or Kr+.
Molecular lasers:
lasing medium is CO2 OR N2.
Excimer lasers:
a gaseous mixture of He, F and one of the rare
gases Argon, Krypton or Xenon.
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20. He/Ne laser has low initial and maintenance
cost, greater reliability, low power consumption
Ar ion laser is a four level device, input energy
is high since Ar has to be ionized then excited
from ground state
InN2 laser excitation is caused by high voltage
spark source, excitation causes population
inversion, which decays quickly
In excimer, rare gas is electronically excited by
a current followed by reaction with flourine to
form excited species ArF*, KrF*
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21. The active materials are solutions of organic
componds capable of fluorescing in UV,IR regions
The dye and solvent are circulated through a cell or
a jet, and the dye molecules are excited by flash
lamps or other lasers.
The organic dye molecules have broad fluorescence
bands and dye lasers are continuously tunable over
20 to 50 nm.
Dyes exist to cover the near-u.v to near-infrared
spectral region: 330 - 1020 nm.
DYE LASERS
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22. LEDs within a resonator cavity that is
formed either on the surfaces of the diode
or externally connected.
Electric current passing through the diode
produces light emission when electrons
and holes recombine at the p-n junction.
The laser output is very divergent and
requires special optics to produce a good
beam shape.
SEMICONDUCTOR LASERS
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23. DBR laser diode
used in optical-fiber communications, CD
players, and in high-resolution molecular
spectroscopy in the near-infrared.
can replace flash lamps to efficiently pump
solid-state lasers.
tunable over a narrow range and different
semiconductor materials are used to make
lasers at 680, 800, 1300, and 1500 nm.
SEMICONDUCTOR LASERS
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25. SOLID STATE LASERS
Ruby crystal is the active medium.
earlier ruby was machined to rod of 4cm
long and .5 cm in diameter
a flash tube( xenon lamp) was cioled
around cylinder to produce intense flashes
of light
thus pulsed radiation was formed
Have very high radiation power at 1064
nm.
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27. IN CHEMISTRY
Analytical chemistry: for ultra sensitive
detection of small concentration of pollutants
Single molecular detection
Laser induced chemical reaction
Isotope separation with lasers
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28. ENVIRONMENTAL RESEARCH
study the pollutants and their reactions with
natural components
Spectroscopic detection of water molecules.
Using photo acoustic spectroscopy with dye
lasers small con. of trans uranium elements
could be detected from ground waters.
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29. IN BIOLOGY
Energy transfer in DNA complex
Time resolved measurement of biological
process.
Laser microscope.
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