HIGH RESOLUTION FOURIER TRANSFORM SPECTROSCOPY OF THE SINGLET MOLECULAR OXYGEN-IODINE REACTION AND POPULATIONS OF THE BOu+B O^{+}_{u} AND A Iu STATES THROUGH NON LINEAR INVERSION OF EMISSION SPECTRA

Abstract

Author Institution: Laboratoire de Specdrometrie lonique et Moleculairs; Laboratokire Aime Cotton, CNRS IIThe dissociation of molecular lodine I2I_{2} by metastable oxygen O2(1Δg)O_{2} (^{1}\Delta_{g}) is poorly understood. It leads to the dissociation of I2I_{2}. Knowledge of this process is important to assessing the ultimate efficiencies of high-power Chemical Oxygen lodine Lasers. In our analysis O2(1Δg)O_{2}(^{1}\Delta_{g}) is obtained from a microwave discharge in oxygen. The flow of less than 10\% of O2(1Δg)O_{2}(^{1}\Delta_{g}) is mixed with pure lodine. The reaction gives a flame emitting from 3700cm13 700 cm^{-1} to 20000cm120000 cm^{-1}. We observe this flame along the axis with a high resolution Fourier Transform spectrometer. The 1000020000cm110000 - 20000 cm^{-1} emission is due to the BOu+xO2+BO^{+}_{u} -xO^{+}_{2} transition and allows to determine the populations of the BOu+BO^{+}_{u} It rovibrational levels.The red region come from Alu.XO9+A lu \rightarrow. X O^{+}_{9} from which we obtain the A 1u populations We have set a general program that gives from non linear least squares fits the rovibrational populations and their statistical errors A 1u serves as a reservoir with a non Boltzmann vibrational distrbition and B O has a maximum population around v=3035v=30-35 The rotational distribution in A1uorBOu+A 1u or B O^{+}_{u} is boltzmann and corresponds to 370±20K370 \pm 20 K. We will give our main results. Our general fitting method will be presented and statistical or systematic errors discussed

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