Rotational and hyperfine structure in the B3Π0+excited state of ICl
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[1] E. Tiemann,et al. Isotopic field shift of the rotational energy of the Pb-chalcogenides and Tl-Halides , 1982 .
[2] E. Tiemann,et al. Observed adiabatic corrections to the born-oppenheimer approximation for diatomic molecules with ten valence electrons , 1982 .
[3] S. Hansen,et al. Microwave-optical double resonance of a supersonic beam: ICI B3Π(O+) v = 0 , 1982 .
[4] E. Tiemann,et al. Hyperfine structure measurements in the B3IIo+u—X 1Σ+g electronic transition of Br2 , 1981 .
[5] M. Broyer,et al. eQq measurements in the X, 1g, O+g and B state of I2: A test of the electronic molecular eigenfunctions , 1980 .
[6] John S. Muenter,et al. Laser fluorescence state selected and detected molecular beam magnetic resonance in I2 , 1980 .
[7] E. Tiemann,et al. Microwave—optical double resonance in the B 3Π0+ excited state of ICl , 1979 .
[8] E. Tiemann,et al. Electric dipole moment of BrCl , 1978 .
[9] D. O. Harris,et al. Microwave optical double resonance of NO2 with a tunable cw dye laser. II. Excited state microwave transitions , 1974 .
[10] D. O. Harris,et al. Microwave optical double resonance spectroscopy with a cw dye laser: BaO X1Σ and A1Σ , 1973 .
[11] E. Herbst,et al. Dipole Moment of ICI , 1972 .