THE PURE ROTATION SPECTRUM OF MOLECULAR HYDROGEN

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1982

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Ohio State University

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Pure rotational quadrupole spectra of H2 were first successfully observed in a source outside the solar system with the detection of emission from the 12.28μm S(2) transition in the Orion nebula1. More recently the high -J transitions S(8), S(9), S(12), S(13), S(14), and S(15) were also observed in Orion.2 The pure rotation spectrum of molecular hydrogen has been recorded in the laboratory using Fourier transform and diode laser spectrometers. Frequencies and quadrupole strengths have been derived for the transitions S(2), S(3), S(4), and S(5) at 12.3, 9, 7, 8.0, and 6.9μm wavelength, respectively. An immediate result of this study was a frequency measurement for the S(2) transition3 originally detected in Orion. The frequency determined, 814.4250cm−1 is different by −0.027cm−1 from the value used in those Orion observations. In addition, this analysis has shown that the usual set of rotational constants B, D, and H are not sufficient for characterizing the ground state rotational levels of H2 up to j=7. The additional constant L is needed to fit the laboratory data (including S(0) and S(1) frequencies obtained from combination differences measured in the vibrational v=0−1 band4). At least five rotational constants are needed to fit both the laboratory measurements and those high-J line frequencies observed in the Orion Molecular Cloud.

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1S.C. Back, J.H Lacy, and T.R., Geballe, Ap. J. (Letters) 234, L213 (1979). 2R.F. Knacke and E.T. Young, Ap. J. (Letters) 242, L183 (1980): also Ap. J. (Letters) 249, L65 (1981). 3D.E. Jennings and J.W. Brault, Ap. J. (Letters), to be published. 4S.L. Bragg, J.W. Brault, and W.B. Smith, to be published.

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