ON ABSORPTION BANDS IN THE KrF LASER SPECTRUM

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1978

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Ohio State University

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Using transverse electric discharges KrF laser spectra were investigated at high resolution under various lasing conditions, and many absorption lines were observed in the laser spectrum in addition, to the absorption between the two peaks at 2484 and 2491 {\AA}. Except for the C I 2478.573 {\AA} absorption from the metastable 2p21S state no possible impurity line or band can be attributed to these absorbing lines, even when two- or three-photon transitions, or absorption from excited states are taken into account. Two series, series I and II, converging to the same limit near 40308cm−1 were found and analyzed as v^{\prime}-progressions of a doublet state. The Δ G-v curves of the series are well represented by straight lines of almost equal slopes, which give ωeXe(I)=2.165 and ωeXe(II)=2.197cm−1 Provided the absorption arises from the upper state of the laser emission, dissociation should occur to Kr(5s[3/2]O)+F(2p5,2P). Assuming the weak series to be due to the isotopic molecule, 86KrF, the following molecular constants were obtained by computer simulation: (The values in parentheses show the ranges of possible deviations due to experimental errors.)[FIGURE]

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Vibrational quantum number estimated for the first member of the observed series. The observed doublet series are so close (within 200cm−1) to the converging limit, that dissociation will easily occur at 300K following absorption. This may play a role in the lasing mechanism, although the total absorption in the half width of the KrF laser, ∼4 {\AA}, was estimated to be less than 5% if the continuous absorption by F2 is disregarded.""


Author Institution: Institute for Optical Research; Faculty of Engineering; Institute of Physics

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