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ANALYTICAL CHEMISTRY



  LASER SPECTROSCOPY
             Ayesha Abdul Ghafoor
                 MS Chemistry
LASER SPECTROSCOPY
   LASER
   Principle of Laser
   Laser System
   Laser as spectroscopic Light source
   Spectroscopy
   LASER +Spectroscopy
       Laser Induced Breakdown Spectroscopy
       Laser Induced Fluorescent Spectroscopy
       Laser ablation inductively coupled plasma optical emission
        spectroscopy (LA-ICP-OES)
       Raman Spectroscopy


   Applications of Laser Spectroscopy
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
L.A.S.E.R
       Light Amplification by Stimulated Emission of Radiation
BASIC LASER

   Light Sources
   Gain medium
   Mirrors


                         I
               I0                  I1


               I3   Laser medium   I2
    R = 100%                            R < 100%
                                              R. Trebino
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
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
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  AN                             BIN  BI N  AN  AN               BIN  BI N  AN
  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)
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
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
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.
LASER SPECTROSCOPY INSTRUMENTATION
   LASER as Source of Light
   Gratings and Monochromators
   Interferometers
       Michelsons Interferometers
       Fourier Transform Spctrometer
     Dtectors
       Thermal Detectors
       Flourescent detectors etc.
   Recorder
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.
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.
   Fig: LIBS Spectra for
    identification of
    different elements in
    sample
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.
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).
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.
   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.
APPLICATIONS OF LASER SPECTROSCOPY

 Medical field
 Analytical Chemistry

 Industrial Applications

 Environmental Applications
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
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
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
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
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
MOLECULES STUDIED IN BREATH BY LASER
SPECTROSCOPY

Molecule                Methods
Acetaldehyde           LIBS , TDLAS
Acetone                   CRDS
Ammonia               PAS, TDLAS, OFC-CEAS
Carbon dioxide       CRDS, TDLAS, CALOS, OFC-CEAS
Carbon monoxide         TDLAS
Carbonyl sulfide       TDLAS, CALOS
D/H isotopic ratio        TDLAS
Ethane                LIBS , OA-ICOS, TDLAS, PAS
Methylamine,             CRDS
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)
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
FIG :RAMAN SPECTRUM OF NATURAL DIAMOND
ARTS ( STUDY OF PAINTING)
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…
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
Questions???
        Glad to Answer your Questions

THANKS FOR LISTNIN

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Laser spectroscopy

  • 1. ANALYTICAL CHEMISTRY LASER SPECTROSCOPY Ayesha Abdul Ghafoor MS Chemistry
  • 2. LASER SPECTROSCOPY  LASER  Principle of Laser  Laser System  Laser as spectroscopic Light source  Spectroscopy  LASER +Spectroscopy  Laser Induced Breakdown Spectroscopy  Laser Induced Fluorescent Spectroscopy  Laser ablation inductively coupled plasma optical emission spectroscopy (LA-ICP-OES)  Raman Spectroscopy  Applications of Laser Spectroscopy
  • 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  AN   BIN  BI N  AN  AN   BIN  BI N  AN 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
  • 29. MOLECULES STUDIED IN BREATH BY LASER SPECTROSCOPY Molecule Methods Acetaldehyde LIBS , TDLAS Acetone CRDS Ammonia PAS, TDLAS, OFC-CEAS Carbon dioxide CRDS, TDLAS, CALOS, OFC-CEAS Carbon monoxide TDLAS Carbonyl sulfide TDLAS, CALOS D/H isotopic ratio TDLAS Ethane LIBS , OA-ICOS, TDLAS, PAS Methylamine, CRDS
  • 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
  • 32. FIG :RAMAN SPECTRUM OF NATURAL DIAMOND
  • 33. ARTS ( STUDY OF PAINTING)
  • 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

Hinweis der Redaktion

  1. Block Diagram of Laser ablation inductively coupled plasma optical emission spectroscopy (LA-ICP-OES)
  2. TDLAS = tunable diode laser absorption spectroscopy, CRDS = cavity ringdown spectroscopy,PAS= phoacoustic spectroscopy, OFC-CEAS = optical frequency comb cavity-enhanced absorptionspectroscopy, CALOS = cavity leak-out spectroscopy, OA-ICOS = off-axis integrated cavityoutput spectroscopy, QEPAS = quartz-enhanced photoacoustic spectroscopy
  3. Industrial application