Results 251 to 260 of about 91,270 (284)
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The Journal of Chemical Physics, 1990
The permanent dipole moment of TiN in its X 2Σ+ and A 2Σ states has been determined from the complete resolution of the first- and second-order Stark splitting of the Q21(1.5)+R2(0.5) line of the (0,0) band of the A 2Π–X 2Σ+ system. Values of 3.56±0.05 D (2σ) and 4.63±0.04 D (2σ) have been derived for the X and A states respectively, from least-squares
B. Simard, H. Niki, P. A. Hackett
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The permanent dipole moment of TiN in its X 2Σ+ and A 2Σ states has been determined from the complete resolution of the first- and second-order Stark splitting of the Q21(1.5)+R2(0.5) line of the (0,0) band of the A 2Π–X 2Σ+ system. Values of 3.56±0.05 D (2σ) and 4.63±0.04 D (2σ) have been derived for the X and A states respectively, from least-squares
B. Simard, H. Niki, P. A. Hackett
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Chemical Physics Letters, 1990
Abstract The electric dipole transition moment has been calculated a priori for the C (1 1 Π u )← X(1 1 Π + g ) electronic transition as a function of R (CC), using ab initio quantum chemical techniques including state averaged, complete active space MCSCF and multireference CI.
James O. Jensen +2 more
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Abstract The electric dipole transition moment has been calculated a priori for the C (1 1 Π u )← X(1 1 Π + g ) electronic transition as a function of R (CC), using ab initio quantum chemical techniques including state averaged, complete active space MCSCF and multireference CI.
James O. Jensen +2 more
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Proceedings of the Royal Society of London. Series A. Mathematical and Physical Sciences, 1965
The nuclear magnetic dipole moments of151Eu and153Eu have been re-measured. The revised values (corrected for diamagnetic shielding) are: μ(151Eu) = 3.4630 ± 0-0006 n.m., μ(153Eu) = 1.5292 ± 0-0008 n.m. The ratio of the moments is μ(151Eu)/μ(153Eu) = 2.26505 ±0.00042. These results were obtained by the method of triple resonance in an atomic beam.
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The nuclear magnetic dipole moments of151Eu and153Eu have been re-measured. The revised values (corrected for diamagnetic shielding) are: μ(151Eu) = 3.4630 ± 0-0006 n.m., μ(153Eu) = 1.5292 ± 0-0008 n.m. The ratio of the moments is μ(151Eu)/μ(153Eu) = 2.26505 ±0.00042. These results were obtained by the method of triple resonance in an atomic beam.
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Electric dipole and quasi-orbital magnetic moments of conduction electrons
Radiophysics and Quantum Electronics, 1967V. N. Genkin, P. M. Mednis
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$$^1$$H, $$^2$$H and $$^3$$H nuclear magnetic dipole moment effects on the electron energy states
Pramana, 2021openaire +1 more source