Xnverse Lamb dips of fGUX transitions of the ND3 PJ baud at 11.4 pm have been measured in a Stark cell @aced inside the cavity of a 13C02 laser. The electric dipole moment of the u2 = 1, (J,K) = (14,ll) and (14.13) states and of the (J,K) = (13.11) and (13.13) states of the vibrational ground state
The electric dipole moment of AsH3 by saturation laser stark spectroscopy
โ Scribed by G. Di Lonardo; L. Fusina; A. Trombetti
- Publisher
- Elsevier Science
- Year
- 1984
- Tongue
- English
- Weight
- 255 KB
- Volume
- 110
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
Inverse Lamb dips of the P(4,3) and R(3.3) transitions of the ~2 band of AsHs at 11 pm have been measured with a Stark cell inside the cavity of a CO* laser. The dipole moments of AsH3 in the ground vibrational state /.Q = 0.217 f 0.003 D and in the ~2 = I state g1 = 0.218 + 0.003 D have been obtained.
๐ SIMILAR VOLUMES
In this work, precise microwave (MW) frequencies were measured for nine different transitions in the three lowest torsional states of \({ }^{13} \mathrm{C}\)-substituted methanol, for a wide range of applied dc electric fields. The Stark shifted frequencies were measured with accuracies of \(\pm 10
PH3 have been brought in resonance with CO2 laser lines. using an intracavity Stark cell. Accurate values of the dipole moments &=, = 0.574Ort 0.0002 D and p,\_=, = 0.5781\* 0.0001 D) and of the transition frequencies have been obtained.
In this paper we report accurate measurements of microwave (MW) frequencies for nine different transitions in the first four torsional states in the ground vibrational state of O-18 substituted methanol, for a wide range of applied dc electric field. The Stark-shifted frequencies were measured with