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Acta Physica Sinica

STIMULATED RAMAN-SCATTERING AND RESONANT LASER-RADIATION IN PHOTODISSOCIATED LEAD ATOMS

J Zhang, By Cheng, Dz Zhang, Lz Zhao, Yy Zhao, Tj Wang

Published Jan 1, 1990• 0 citations
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Abstract

Strong stimulated radiation at wavelengths 3740 A was observed when PbCl 2 molecules were photodissociated by a 2660 A UV laser. Based on spectral characteristics and Pb energy level structure, this radiation was judged to be resonant laser radiation and stimulated Raman scattering due to the populated 6p 2 3 P 2 metastable Pb atoms from photodissociated PbCl 2 molecules. A theoretical model was developed to describe the whole process, and experimentally fitted to determine the photodissociation coefficient of the metastable Pb atoms from dissociated PbCl 2 by 2660 A laser

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The Journal of Chemical Physics•Mar 1, 1982•2 citations
Strong stimulated radiation at wavelengths 3740 A was observed when PbCl 2 molecules were photodissociated by a 2660 A UV laser. Based on spectral characteristics and Pb energy level structure, this radiation was judged to be resonant laser radiation and stimulated Raman scattering due to the populated 6p 2 3 P 2 metastable Pb atoms from photodissociated PbCl 2 molecules. A theoretical model was developed to describe the whole process, and experimentally fitted to determine the photodissociation coefficient of the metastable Pb atoms from dissociated PbCl 2 by 2660 A laser
Strong stimulated radiations at wavelengths 3740 A have been observed when PbCl2 molecules are photodissociated by 2660 A ultraviolet laser. Dependences of these radiations on the pump laser intensity and PbCl2 molecular density have been studied experimentally. A theoretical model to describe these processes is put forward. These two raditions are identified as resonant laser radiation and stimulated Raman scattering originated from bhe population of the metastable level 6p23P2 of atomic Pb, which is produced by two-photon dissociation of PbCl2. When molecular density of PbCl3 is 6.21×1016cm-3, the maximum populations on the two metastable levels, 6p23 P2 and 6p21D2, of atomic Pb are almost same, which equals 2.0×1016cm-3.
A large number of Ti atoms populated mainly on the ground state (a3F2) and metastable states (a3F3,4) were produced by UV-laser (259-300 nm) photodissociation of TiCl4. Many stimulated Raman scattering lines and stimulated radiations of Ti atoms were observed by pumping Ti atoms on the a3F2,3,4 states via nearly resonant transitions. All the lines observed were assigned. The pulse duration and timeresolved spectrum of SRS of Ti atoms shows the photolysis of TiCl4 to Ti atom was very fast, and the time estimated for it was less than Ins.
Under excitation of 355nm or 266nm UV radiation some strong emissions have been observed in PbI 2 vapor. Analysis shows that they are 1st, 2nd order Stokes and 1st anti-Stokes components of 355nm laser and 1st order Stokes and anti-Stokes components of 266nm laser. The initial states of Raman transition are 6p 2 3 P 1 and 6p 2 3 P 2 metastable states of atomic Pb, respectively. The population on it is created by photodissociation of PbI 2 . The dependences of Raman components on pump power, PbI 2 density and pressure of buffer gas are investigated experimentally.
The population on 6p2 3P2 metastable state and 6p2 3P0 ground state of Pb atoms are de-monstrated, which are originated from dissociating PbCl2 by the fourth harmonic of YAG lasers. The population ratio of 3P2 to 3P0 is measured in terms of laser-induced fluorescence. The results indicate that the dissociation of PbCl2 is a two photon process and the population inversion between 3P2 and 3P0 exists. The stimulated Raman radiation based on the population of 3P2 metastable state is observed. The possible way of dissociation is studied.