3. 2013-2-26
FLASHES OF BRILLIANCE
THE HISTORY OF THE LASER
“A splendid light has dawned on me”
– Albert Einstein
In 1917 Einstein published ideas on stimulated emission of radiation.
The laser is credited as being invented in 1958 by Charles H. Townes and
Arthur L. Schawlow. Townes coined the term “laser” with help from his
students.
On May 16, 1960, Theodore H. Maiman operated the first functioning
laser i.e., a pulse mode operation of solid- state flash lamp -pumped
4. L.A.S.E.R
Light Amplification by Stimulated Emission of Radiation
5. BASIC LASER
Light Sources
Gain medium
Mirrors
I
I0 I1
I3 Laser medium I2
R = 100% R < 100%
R. Trebino
6. GAIN MEDIUM
Einstein Coefficients
E2
AN2 = rate of Spontaneous emission
E1
E2
BN2I = rate of Stimulated emission
E1
E = hν
E2
BN1I = rate of Stimulated absorption
E1
7. TO ACHIEVE LASING:
Stimulated emission must occur at a
maximum (Gain > Loss)
Loss:
Stimulated Absorption
Scattering, Reflections
Energy level structure must allow for
Population Inversion
E2
E1
8. OBTAINING POPULATION INVERSION
2-level system 3-level system 4-level system
3 3
Fast decay Fast decay
2 2
2 N2
I sat Pump Laser Pump Laser
Laser Transition Transition Transition Transition
1 N1 1 1
Fast decay
0
d N d N d N
2 BI N AN AN BIN BI N AN AN BIN BI N AN
dt dt dt
N 1 I / I sat I / I sat
N N N N N
1 I / I sat 1 I / I sat 1 I / I sat
Population Inversion is obtained for ΔN < 0 (ΔN = N1 – N2)
9. LASER SYSTEM
Active Medium 3
Active medium can be of following types
Liquid Fast decay
Solid 2
gases
Pumping Source Pump Laser
Optical pumping Transition Transition
Chemical pumping
Nuclear pumping
Discharge technique 1
Laser pumping Fast decay
Electron beam pimping 0
Resonators
Transverse Mode
Longitudinal mode
10. Tunnable Lasers
wavlength of operation can be altered in controlled manner.
Dye lasers use complex organic dyes
Gas lasers are pumped by current.
Solid-state lasers have lasing material distributed in a solid matrix
(such The Nd:YAG laser emits infrared light at 1.064 nm.
Semiconductor lasers, sometimes called diode lasers, are p-n
junctions. Current is the pump source. Applications: laser printers or
CD players.
Excimer lasers (from the terms excited and dimers) use reactive
gases, such as chlorine and fluorine, mixed with inert gases such as
argon, krypton, or xenon. Excimers lase in the UV.
Free electron Lasers is a laser that shares the same opical
properties as conventional lasers such as emitting a beam of
coherent EMR radiations which can reach high power
R. Trebino
11. SPECTROSCOPY
Study of interaction of light with matter
all atoms and molecules absorb and emit
light at certain wavelengths so we can
identify and read their properties
In essence, every element has a unique
atomic "fingerprint" that takes the form of a
set of wavelengths, or a spectrum.
12. LASER SPECTROSCOPY INSTRUMENTATION
LASER as Source of Light
Gratings and Monochromators
Interferometers
Michelsons Interferometers
Fourier Transform Spctrometer
Dtectors
Thermal Detectors
Flourescent detectors etc.
Recorder
13. LASER-INDUCED BREAKDOWN
SPECTROSCOPY (LIBS)
advanc-ing significantly over the last decade.
It can analyze solids, liquids and gases and
can return results rapidly, with very little
damage to the sample.
It can do its work from a distance, unlike
some analytical tools that require samples
being brought to a lab.
14. WORKING OF LIBS
The laser, of course, Generally, LIBS systems use a
neodymium-doped yttrium aluminum garnet
(Nd:YAG) laser at fundamental wavelength of 1,064
nanometers
(but many different lasers have been used. The laser
doesn't blast the sample with a nonstop beam)
The laser light passes through a lens, which focuses the
energy onto the sample.
"laser spark” produced.
Excitation
Relaxation
The spectrometer contains a prism and a camera to
photograph the spectra for further study.
15.
16. Fig: LIBS Spectra for
identification of
different elements in
sample
17. LASER ABLATION INDUCTIVELY COUPLED
PLASMA OPTICAL EMISSION SPECTROSCOPY
(LA-ICP-OES)
The "P" in ICP stands for plasma, an ionized gas
consisting of positive ions and free electrons.
The Plasma torch consists of three concentric tubes
of silica surrounded by a metal coil. A nozzle at the
end of the torch acts as an exit for the plasma.
Now the instrument is ready to analyze a sample.
In the laser-based version of ICP-OES, a
neodymium-doped yttrium aluminum garnet (Nd:YAG)
laser is used to cut, or ablate, a few microscopic
particles from the sample's surface. The ablated
particles are then carried to the pl-asma torch, where
they become excited and emit light.
18.
19. LASER-INDUCED FLUORESCENCE (LIF)
Laser-induced fluorescence (LIF) is a spectroscopic
method used for studying structure of molecules,
detection of selective species and flow visualization and
measurements.
Experimental Method
The species to be examined is excited with a laser. The
wavelength is often selected to be the one at which the
species has its largest cross section . The excited species
will after some time, usually in the order of few
nanoseconds to microseconds, de-excite and emit light at
a wavelength longer than the excitation wavelength. This
fluorescent light is typically recorded with a
photomultiplier tube (PMT).
20.
21. RAMAN SPECTROSCOPY
C.V. Raman ,Indian scientist discovered Raman
spectroscopy
Raman spectroscopy is a spectroscopic technique used to
study vibrational , rotational, and other low-frequency modes
in a system
Principle: It relies on inelastic scattering , or Raman scattering,
of monochromatic light, usually from a laser in the visible ,
near infrared , or near ultraviolet range. The laser light
interacts with molecular vibrations, phonons or other
excitations in the system, resulting in the energy of the laser
photons being shifted up or down. This happens because the
laser light interacts with phonons. The shift in energy gives
information about the phonon modes in the system and
ultimately about the molecules present in the sample.
22. Experimental Procedure: The
beam from an argon-ion laser is
directed by a system of mirrors
to a lens, which focuses
monochromatic light onto the
sample. Most of the light
bouncing off the sample
scatters at the same
wavelength as the incoming
light, but some of the light does
scatter at different wavelengths
and goes to detector This
happens because the laser light
interacts with phonons. we use
photomultiplier ,CCD detectors
etc. and determine vibrations
kinds and finally sample
molecule.
23. APPLICATIONS OF LASER SPECTROSCOPY
Medical field
Analytical Chemistry
Industrial Applications
Environmental Applications
24. LASER SPECTROSCOPY IN MEDICINE AND
BIOLOGY
Medical diagnostics by breath trace gas analysis
Real-time monitoring of exhaled gases (therapeutic monitoring,
toxicology, occupational health)
Tissue analysis
Mapping of drug delivery
Insect studies
Plant physiology
25. IDENTIFICATION OF BACTERIAL
CONTAMINATION OF PLATELETS (LIF)
Blood transfusion carries a risk of
infection (hepatitis, HIV…) or
consequent sepsis
every platelet concentrate should be
checked before use (after donation and
shortly before transfusion
» Fluorescent stain attaches to the DNA of
bacteria (platelets don’t contain DNA!)
» Frequency doubled Nd-laser (532 nm)
to
excite LIF
» Scattered light also measured
» Certain thresholds for both signals
26. REAL-TIME MONITORING
Real-time monitoring OF HEMODIALYSIS
of hemodialysis
» Hemodialysis is used
in treatment of renal
failure
» Urea, creatinine, etc.
removed
» Treatment 3 times a
week, 2-12 hours
» Over million patients
worldwide, growing fast
27. LIF SPECTROSCOPY OF TISSUES
There are cellular or
subcellular differences
between normal and
tumorous tissues
» LIF can be used to
visualize tissue
characteristics
and detection of anomalies
» Fluorescing compounds
or autofluorescence
» Non-invasive procedure,
no photosensitization or
photodestruction
28. RESPIRATION OF INSECTS
Respiration of insects
- real-time, on-line measurement of
CO2
- very small quantities sensitive
detection method, small volume of
sample line and cell
photoacoustic spectroscopy
- mid-IR should be used if possible
(CO2 at 4.234 μm)
- OPO (between 3.9 and 4.8 μm)
continuous-wave, single mode
operation
- detection limit 0.7 ppb.
- sporadic release of CO2 observed
30. LASER SPECTROSCOPY OF BREATH IS
LIMITED TO SMALL MOLECULES
single vibration-rotation
lines are measured
-the lines have a certain
linewidth (Voigt profile)
-the bigger the molecules,
the more congested the
spectrum becomes(lines
start to overlap
each other)
-typical laser wavelength 1.5
to 10 μm
-sensitivity ppt – ppm
-normal pressure cannot
usually be used (typical p =
0.05 – 0.2 atm)
31. IN ANALYTICAL CHEMISTRY
Laser Spectroscopy in Analytical Chemistry
Chemical Reactions
Detection of Atoms
Study of Transition States
Separation of isotopes (In Nuclear Reactors)
Study of Bond Energies and Angles
Type of Material
34. LIF SPECTROSCOPY OF INTERNAL COMBUSTION
ENGINES
LIF spectroscopy of internal
combustion engines
Goals: to improve combustion
efficiency to reduce emission of
pollutants
how well air and fuel are mixed
chemical intermediates
rate constants of key reactions
l = air/fuel ratio
ArF ,KrF lasers
Molecules:
NO, CO, CO2, hydrocarbons…
35. CONCLUDING THOUGHTS
The key to managing today’s rapidly evolving technology it to
constantly analyze how each advance affects us as individuals
and as a society as a whole. “
“Our Advancing Technology , if separated from the
human factor, I take to be part of the advance in the evolving
quality of existence, something that gives added meaning and
higher dimension to the human venture…”
- Roger Sperry
Neuroscientist and Nobel Laureate
36. Questions???
Glad to Answer your Questions
THANKS FOR LISTNIN