Abstract
The emission spectrum of iodine (I2) between 5000 and 2500 A. consists of a large number of diffuse bands (McLennan bands) and, especially in the presence of small amounts of an inert gas, of some apparently structureless continua1 at 4800, 4300 and 3420 A. However, as has been shown, particularly by Elliott2, the spectrum has quite a different appearance if excited in fluorescence by the Al spark lines at 1855–1863 A. in the presence of large amounts of nitrogen. The McLennan bands disappear almost entirely, the continua change into well-developed band systems at 4630–4440, 4321–4041(E) and 3450–3040 A.(D), and another well-developed band system appears at 2730–2520 A.( F). From a vibrational analysis of system D, Elliott was able to confirm an earlier interpretation of this system as an electronic transition from an upper state 1Σ+u to the ground state 1Σ+g of I2 (with vibrational quantum numbers v″ = 13—29). He also set up a formula for system F, but his v″-assignment is uncertain, and indeed entirely incorrect according to our analysis. He was unable to interpret the other two systems.
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References
A good survey is given by Curtis, W. E., and Evans, S. F., Proc. Roy. Soc., A, 141, 603 (1933). See also Venkateswarlu, P., Proc. Ind. Acad. Sci., A, 24, 480 (1946).
Elliott, A., Proc. Roy. Soc., A, 174, 273 (1940).
Loomis, F. W., Phys. Rev., 29, 112 (1927). Mecke, R., Ann. Phys., 71, 104 (1923).
Mulliken, R. S., Phys. Rev., 46, 549 (1934).
Wieland, K., Helv. Phys. Acta, 14, 420 (1941). See also Victor Henri Memorial Volume (Liège, in the press).
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WASER*, J., WIELAND, K. Emission Spectrum of Iodine Molecules in the Presence of an Inert Gas. Nature 160, 643–644 (1947). https://doi.org/10.1038/160643b0
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DOI: https://doi.org/10.1038/160643b0
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