-
2
-
-
0038302547
-
-
K. R. Leopold, G. T. Fraser, S. E. Novick, and W. Klemperer, Chem. Rev. 94, 1807 (1994).
-
(1994)
Chem. Rev.
, vol.94
, pp. 1807
-
-
Leopold, K.R.1
Fraser, G.T.2
Novick, S.E.3
Klemperer, W.4
-
3
-
-
0348164027
-
-
J. Kommandeur, W. A. Majewski, W. L. Meerts, and D. W. Pratt, Annu. Rev. Phys. Chem. 38, 443 (1987).
-
(1987)
Annu. Rev. Phys. Chem.
, vol.38
, pp. 443
-
-
Kommandeur, J.1
Majewski, W.A.2
Meerts, W.L.3
Pratt, D.W.4
-
12
-
-
0032529985
-
-
B. H. Pate, J. Chem. Phys. 109, 4396 (1998), preceding paper.
-
(1998)
J. Chem. Phys.
, vol.109
, pp. 4396
-
-
Pate, B.H.1
-
18
-
-
11644279404
-
-
V. N. Bagratashvili, S. I. Ionov, A. A. Stuchebrukhov, V. S. Letokhov, V. N. Lokhman, and G. N. Makarov, Chem. Phys. Lett. 146, 599 (1988).
-
(1988)
Chem. Phys. Lett.
, vol.146
, pp. 599
-
-
Bagratashvili, V.N.1
Ionov, S.I.2
Stuchebrukhov, A.A.3
Letokhov, V.S.4
Lokhman, V.N.5
Makarov, G.N.6
-
20
-
-
0001751778
-
-
E. Hudspeth, D. A. McWhorter, and B. H. Pate, J. Chem. Phys. 109, 4316 (1998), this issue.
-
(1998)
J. Chem. Phys.
, vol.109
, pp. 4316
-
-
Hudspeth, E.1
McWhorter, D.A.2
Pate, B.H.3
-
21
-
-
22244440457
-
Double-resonance spectroscopy of molecules by means of lasers
-
in edited by H. Walther Springer-Verlag, New York
-
K. Shimoda, "Double-resonance spectroscopy of molecules by means of lasers," in Laser Spectroscopy of Atoms and Molecules, edited by H. Walther (Springer-Verlag, New York, 1976).
-
(1976)
Laser Spectroscopy of Atoms and Molecules
-
-
Shimoda, K.1
-
22
-
-
22244456319
-
Infrared-microwave double resonance
-
in edited by R. G. Brewer and A. Mooradian Plenum, New York
-
K. Shimoda, "Infrared-microwave double resonance", in Laser Spectroscopy, edited by R. G. Brewer and A. Mooradian (Plenum, New York, 1974).
-
(1974)
Laser Spectroscopy
-
-
Shimoda, K.1
-
25
-
-
22244432440
-
-
A fit of the rotational constants to the centers of each rotational IVR multiplet in the infrared spectrum (Ref. 20) was performed. Only the rotational constants were varied. The change in 1 2 (B+C) for the acetylenic C-H bright state was determined to be 8 MHz with a standard deviation, σ=4MHz
-
A fit of the rotational constants to the centers of each rotational IVR multiplet in the infrared spectrum (Ref. 20) was performed. Only the rotational constants were varied. The change in 1 2 (B+C) for the acetylenic C-H bright state was determined to be 8 MHz with a standard deviation, σ=4MHz.
-
-
-
-
27
-
-
0001417040
-
-
A. McIlroy, D. J. Nesbitt, E. R. Th. Kerstel, K. K. Lehmann, B. H. Pate, and G. Scoles, J. Chem. Phys. 100, 2596 (1994).
-
(1994)
J. Chem. Phys.
, vol.100
, pp. 2596
-
-
McIlroy, A.1
Nesbitt, D.J.2
Kerstel, E.R.Th.3
Lehmann, K.K.4
Pate, B.H.5
Scoles, G.6
-
28
-
-
0001011658
-
-
J. E. Gambogi, E. R. Th. Kerstel, X. Yang, K. K. Lehmann, and G. Scoles, J. Mol. Spectrosc. 175, 198 (1996).
-
(1996)
J. Mol. Spectrosc.
, vol.175
, pp. 198
-
-
Gambogi, J.E.1
Kerstel, E.R.Th.2
Yang, X.3
Lehmann, K.K.4
Scoles, G.5
-
29
-
-
0001077721
-
-
-1. For the simulations, one-third of this value is used to account for fluctuations in the spectral intensities
-
-1. For the simulations, one-third of this value is used to account for fluctuations in the spectral intensities: E. J. Heller, J. Chem. Phys. 92, 1718 (1990).
-
(1990)
J. Chem. Phys.
, vol.92
, pp. 1718
-
-
Heller, E.J.1
-
34
-
-
22244455682
-
-
The ground state value of 1 2 (B+C) is 8932.5 MHz (unpublished results from microwave measurements of the pure rotational spectrum of propynol in our spectrometer)
-
The ground state value of 1 2 (B+C) is 8932.5 MHz (unpublished results from microwave measurements of the pure rotational spectrum of propynol in our spectrometer).
-
-
-
|