LASER INDUCED PHOTOACOUSTIC SPECTROSCOPYLIPAS OF RARE EARTH IONS - PowerPoint PPT Presentation

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LASER INDUCED PHOTOACOUSTIC SPECTROSCOPYLIPAS OF RARE EARTH IONS

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1970's: Allan Rosencwaig and Allen Gersho laid the basis ... Then adjusted to a certain concentration with distilled water. 7. Apparatus. 8. Apparatus contd... – PowerPoint PPT presentation

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Title: LASER INDUCED PHOTOACOUSTIC SPECTROSCOPYLIPAS OF RARE EARTH IONS


1
LASER INDUCED PHOTOACOUSTIC SPECTROSCOPY(LIPAS)
OF RARE EARTH IONS IN AQUEOUS SOLUTIONS

SHRUTI PADHEE 27 NOV 2008
2
History
  • 1881 A.G Bell proposed spectrophone ,to examine
    absorption spectra of bodies in those portions
    of the spectrum that are invisible.
  • 1970s Allan Rosencwaig and Allen Gersho laid
    the basis for photo acoustic effect in solids
    called R-G theory

3
What is photo acoustic (PA) spectroscopy?
  • PA spectroscopy is an indirect absorption
    measurement.
  • Here the absorption of light causes a change in
    the temperature or a parameter related to
    temperature (pressure or density) .
  • The heating of the sample produces a PA signal
    correlated directly to absorbed electromagnetic
    energy.
  • When temperature rise in the sample occurs faster
    than its volume can expand local pressure wave
    is generated (considered as sound signal)

4
The Main principle
5
Photo acoustic laser spectra vs Absorption
spectra
  • PA is useful to measure extremely weak
    absorptions (forbidden transitions of rare earth
    ions in liquid).
  • PA can detect radiation less decay processes.
  • Spectra for a turbid or a solid sample can be
    obtained.
  • Background noise can be decreased in PA
    spectroscopy.
  • PA has better detection limit than Absorption
    spectroscopy.

6
Experimental reagents
  • Transition earth metals (Pr, Nd, Eu, Ho, Er)
  • Rare earth nitrates were prepared by dissolving
    the oxides(99.9) in nitric acid.
  • Then adjusted to a certain concentration with
    distilled water.

7
Apparatus
8
Apparatus contd
  • Tunable dye laser pumped by argon ion laser
    (modulated at 200 Hz by light chopper)
  • Dyes used Rhodamine(110,6G,B)-?-540-600,
    570-630, 600-670nm)
  • Band width of dye laser-1cm-1
  • Power of laser dye 300 mW.
  • Pressure fluctuation detected by piezoelectric
    ceramic.
  • 90mm cell length, all measurements at room
    temperature .

9
Praseodymium ion(Pr3) _at_ 590nm
  • E.configuration4f3 6s2
  • Ion 4f2
  • Transition from 3H4 to 1D2.
  • Fine structure obtained as compared to absorption
    spectra.
  • Splitting due to stark effect.
  • the 1D2 splits ,µ _2,_1,0

10
Neodymium ion(Nd3)_at_575 and 625 nm
  • E.configuration4f4 6s2
  • Ion 4f3
  • Transitions4I9/2 to 2G ,4G(mixed) and 2H11/2 .
  • Fine structures were seen in PA and not in
    absorption spectra.
  • In aqueous solutions these ions undergo rapid
    radiation less relaxation.

11
Europium ion(Eu3)_at_579nm
  • E.configuration4f7 6s2
  • Ion4f6
  • Transition4F0 to 5D0
  • Europium fluoresces a
  • lot at 613nm therefore
  • if conc. below 0.1 M are considered then PA
  • spectrum cannot be clearly observed.

12
Holmium ion (Ho3)_at_540 nm
  • E.configuration 4f11 6s2
  • Ion 4f10
  • Transition 5I8 to 5F4 and 5S2
  • Due to the limiting wavelength of dyes used PA
    could not be observed over a whole wavelength
    range.
  • Only slight difference between the absorption and
    the PA spectra due to different cascade processes.

13
Erbium ion(Er3)_at_542nm and 652nm
  • E.configuration4f14 6s2
  • Ion4f13
  • Transition
  • 542nm4I15/2 to 4S
  • 652nm4I15/2 to 4F9/2
  • Both spectra were not clear due to limiting
    lasing wavelength.

14
Conclusions
  • PA is a simple spectroscopy method .
  • PA spectra can give spectral measurements of
    extremely weak absorption.
  • Can be used for variety of samples in gases or
    in solid phase.
  • Useful for substances with very high molar
    absorptivities.

15
Advantages of having lasers as light source
  • The PA signal is proportional to temperature rise
    in sample ,thus proportional to absorbed energy
    (pulse energy)
  • Selectivity of a PA analysis depends on the
    bandwidth of excitation energy.

16
Disadvantages
  • Compounds that fluoresce a lot cannot be detected
    by the photo acoustic spectroscopy as the PA
    signal is directly proportional to the amount of
    heat released by the sample. (if there is more
    fluorescence then there is less heat released by
    the molecule, hence PA signal is not detected)

17
Applications
  • Quantification of soot particles in diesel engine
    exhaust gas.
  • Analysis of highly concentrated textile dyes.
  • Atmospheric pollution monitoring.

18
Expected exam Question
  • What are the advantages of PA spectroscopy over
    absorption spectroscopy?
  • Look at slide 5

19
References
  • Sawada ,T. Oda, S. Shimizu,H. and Kamada, H.
    , Analytical chemistry (1979),vol 51 no.6.
  • Haish,C. and Niessner ,Institute of
    Hydrochemistry, Technical university of Munich
    ,Germany.

20
Thank you DR.CEDENO and the Audience

21
Any questions???
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