Abstract
THE introduction of barium salts to flames or arcs leads, in presence of oxygen, to the production of a characteristic band-spectrum attributed to BaO. Mecke and Guillery1 derived a band-head equation. Mahanti2 gave a new vibrational analysis and also made a rotational analysis. From this the spectrum was shown to arise from a 1Σ–1Σ transition with B' e = 0·30995, B" e = 0·36440 cm.-1 and r"e = 1·787 X 10-8 cm. On checking Mahanti's data, several discrepancies became apparent. Thus some of the plots of 2v0 against J2, [2v0≃R(J-1) + P(J) 2(B – B') J2 show anomalous changes of slope, some of the Combination differences agree rather poorly, and the usual graphical method for determination of B, namely, by plotting Δ"2F(J)/ (J + ½) against (J + ½)2, gives for B2 another value than that quoted by Mahanti. These facts were disclosed by James3, who, from some relatively low-dispersion plates, was able to suggest an alternative rotational analysis with B" 0·31, B'≃0·26 cm.'1.
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References
Mecke, R., and Guillery, M., Phys. Z., 28, 514 (1928).
Mahanti, P. C., Proc. Phys. Soc., 46, 51 (1934).
James, J. A., B.A. thesis, Oxford (1947).
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LAGERQVIST, A., LIND, E. & BARROW, R. Band-Spectrum of Barium Oxide. Nature 164, 923–924 (1949). https://doi.org/10.1038/164923b0
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DOI: https://doi.org/10.1038/164923b0
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