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13
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21144471201
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G. T. Fraser, B. H. Pate, G. A. Bethardy, and D. S. Perry, Chem. Phys. 175, 223 (1993).
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(1993)
Chem. Phys.
, vol.175
, pp. 223
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Fraser, G.T.1
Pate, B.H.2
Bethardy, G.A.3
Perry, D.S.4
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19
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0000004107
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S. Cupp, C. Y. Lee, D. A. McWhorter, and B. H. Pate, J. Chem. Phys. 109, 4302 (1998), this issue.
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J. Chem. Phys.
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Cupp, S.1
Lee, C.Y.2
McWhorter, D.A.3
Pate, B.H.4
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22
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22244490930
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(unpublished results). The dipole moment components of propynol were measured using the molecular Stark effect on a Fourier transform microwave (FTMW) spectrometer at NIST, Gaithersburg. Additional high frequency microwave transitions were measured using a Stark cell spectrometer
-
F. J. Lovas, R. D. Suenram, M. Y. Tretyakov, G. T. Fraser, and B. H. Pate (unpublished results). The dipole moment components of propynol were measured using the molecular Stark effect on a Fourier transform microwave (FTMW) spectrometer at NIST, Gaithersburg. Additional high frequency microwave transitions were measured using a Stark cell spectrometer.
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Lovas, F.J.1
Suenram, R.D.2
Tretyakov, M.Y.3
Fraser, G.T.4
Pate, B.H.5
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24
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22244468288
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See AIP Document No. E-PAPS: E-JCPSA6-109-018835* for a complete listing of transition frequencies and intensities of the acetylenic CH and OH stretch spectra. E-PAPS document files may be retrieved free of charge from our FTP server (http://www.aip.org/epaps/epaps.html) or from ftp.aip.org in the directory /epaps/. For further information: e-mail: paps@aip.org or fax: 516-576-2223.
-
See AIP Document No. E-PAPS: E-JCPSA6-109-018835 for a complete listing of transition frequencies and intensities of the acetylenic CH and OH stretch spectra. E-PAPS document files may be retrieved free of charge from our FTP server (http://www.aip.org/epaps/epaps.html) or from ftp.aip.org in the directory /epaps/. For further information: e-mail: paps@aip.org or fax: 516-576-2223.
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25
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22244485954
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Several separate microwave searches have been performed to identify transitions from a second conformer (expected to be the trans conformation). These measurements have used Stark cell spectrometers [Refs. 21, 22, and (private communication)], a FTMW spectrometer (Ref. 22), and the EROS. No transitions that can be assigned to a second conformation have been found
-
Several separate microwave searches have been performed to identify transitions from a second conformer (expected to be the trans conformation). These measurements have used Stark cell spectrometers [Refs. 21, 22, and J. C. Pearson (private communication)], a FTMW spectrometer (Ref. 22), and the EROS. No transitions that can be assigned to a second conformation have been found.
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Pearson, J.C.1
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26
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22244451614
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Many of the molecules previously studied by high-resolution molecular-beam spectroscopy do not meet the single bright-state criterion. In particular, the high barrier to methyl group internal rotation produces an overlapping spectrum of the noninteracting A and E symmetry states (Ref. 10)
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Many of the molecules previously studied by high-resolution molecular-beam spectroscopy do not meet the single bright-state criterion. In particular, the high barrier to methyl group internal rotation produces an overlapping spectrum of the noninteracting A and E symmetry states (Ref. 10).
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32
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33645724878
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A lengthening of the effective Golden Rule decay rate by this type of level structure has been discussed previously;
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A lengthening of the effective Golden Rule decay rate by this type of level structure has been discussed previously; G. A. Voth, J. Chem. Phys. 88, 5547 (1988).
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Voth, G.A.1
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0032529978
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A. M. Andrews, G. T. Fraser, and B. H. Pate, J. Chem. Phys. 109, 4290 (1998), this issue.
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Andrews, A.M.1
Fraser, G.T.2
Pate, B.H.3
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35
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0001017304
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E. R. Th. Kerstel, K. K. Lehmann, T. F. Mentel, B. H. Pate, and G. Scoles, J. Phys. Chem. 95, 8282 (1991).
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Kerstel, E.R.Th.1
Lehmann, K.K.2
Mentel, T.F.3
Pate, B.H.4
Scoles, G.5
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37
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36449004500
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A. McIlroy, D. J. Nesbitt, E. R. Th. Kerstel, B. H. Pate, K. K. Lehmann, and B. H. Pate, J. Chem. Phys. 100, 2596 (1994).
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McIlroy, A.1
Nesbitt, D.J.2
Kerstel, E.R.Th.3
Pate, B.H.4
Lehmann, K.K.5
Pate, B.H.6
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40
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0007084071
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G. M. Stewart, M. D. Ensminger, T. J. Kulp, R. S. Ruoff, and J. D. McDonald, J. Chem. Phys. 79, 3190 (1983).
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Stewart, G.M.1
Ensminger, M.D.2
Kulp, T.J.3
Ruoff, R.S.4
McDonald, J.D.5
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41
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0001600990
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More detailed modeling of the effects of Coriolis interactions are possible using the methods developed by Perry;
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More detailed modeling of the effects of Coriolis interactions are possible using the methods developed by Perry; D. S. Perry, J. Chem. Phys. 98, 6665 (1993), and Ref. 15.
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J. Chem. Phys.
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Perry, D.S.1
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44
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22244471622
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In the prolate symmetric top limit, the K=0 states would only experience perpendicular Coriolis interactions. The rotational dependence of the perpendicular Coriolis interaction is used in the simulation (for the case where K=0)
-
In the prolate symmetric top limit, the K=0 states would only experience perpendicular Coriolis interactions. The rotational dependence of the perpendicular Coriolis interaction is used in the simulation (for the case where K=0);
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45
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0003539113
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Wiley, New York
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W. Gordy and R. L. Cook, Microwave Molecular Spectra, Techniques of Chemistry (Wiley, New York, 1984), Vol. XVIII.
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Gordy, W.1
Cook, R.L.2
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