Results 271 to 280 of about 116,471 (292)
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Dipole and solenoidal magnetic moments of electronic surface currents on toroidal nanostructures
Journal of Computer-Aided Materials Design, 2007The time-dependent Schrodinger equation is developed for a spinless electron which is confined to move on a toroidal surface and curvature effects are taken into account. The electron motion is driven by linearly or circularly polarized microwaves including an interference field.
Mark Jack, M. Encinosa
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Theory of electron density in a collisionless plasma in the vicinity of a magnetic dipole
Physics of Plasmas, 2018This paper first points out that experimental models of weak lunar swirls and studies of magnetized dusty plasma crystals are linked by the same underlying electron physics.
J. Gibson, M. Coppins
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The Journal of Chemical Physics, 1988
The technique of intermodulated fluorescence has been utilized to record the sub-Doppler optical spectrum of gas-phase copper monosulfide, CuS. The magnetic hyperfine interactions in the A 2Σ−(v=0) and X 2Πi(v=0) states have been analyzed and the permanent electric dipole moment for the X 2Πi state determined.
David F. Nachman+3 more
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The technique of intermodulated fluorescence has been utilized to record the sub-Doppler optical spectrum of gas-phase copper monosulfide, CuS. The magnetic hyperfine interactions in the A 2Σ−(v=0) and X 2Πi(v=0) states have been analyzed and the permanent electric dipole moment for the X 2Πi state determined.
David F. Nachman+3 more
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Bulletin of the Russian Academy of Sciences: Physics, 2008
We have derived and investigated analytical expressions for the cross sections and spin asymmetries in the elastic electromagnetic and electroweak scattering of unpolarized/longitudinally polarized electrons on a polarized/unpolarized proton target with allowance for the C-, P-, and T/CP-invariance violating anapole and electric dipole moments, as well
M. Ya. Safin, B.K. Kerimov
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We have derived and investigated analytical expressions for the cross sections and spin asymmetries in the elastic electromagnetic and electroweak scattering of unpolarized/longitudinally polarized electrons on a polarized/unpolarized proton target with allowance for the C-, P-, and T/CP-invariance violating anapole and electric dipole moments, as well
M. Ya. Safin, B.K. Kerimov
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Journal of Chemical Theory and Computation, 2019
An implementation of transition-dipole moments at the equation-of-motion coupled-cluster singles-doubles (EOM-CCSD) and CCSD linear response (LR) levels of theory for the treatment of atoms and molecules in strong magnetic fields is presented. The presence of a finite magnetic field leads, in general, to a complex wave function and a gauge-origin ...
Florian Hampe, Stella Stopkowicz
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An implementation of transition-dipole moments at the equation-of-motion coupled-cluster singles-doubles (EOM-CCSD) and CCSD linear response (LR) levels of theory for the treatment of atoms and molecules in strong magnetic fields is presented. The presence of a finite magnetic field leads, in general, to a complex wave function and a gauge-origin ...
Florian Hampe, Stella Stopkowicz
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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
Benoit Simard, Peter A. Hackett, H. Niki
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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
Benoit Simard, Peter A. Hackett, H. Niki
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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.
Cary F. Chabalowski+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.
Cary F. Chabalowski+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.
L. Evans+2 more
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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.
L. Evans+2 more
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Physical Review C, 2018
Magnetic dipole and electric quadrupole moments are calculated for neutron-rich sd-pf cross-shell nuclei. These nuclei include open shell isotopes with the number of protons less than 20 and neutrons greater than 20, for which experimental data are available. Shell model calculations are performed with full $sd$ shell model space for $Z$\ensuremath{-}8
R. A. Radhi+2 more
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Magnetic dipole and electric quadrupole moments are calculated for neutron-rich sd-pf cross-shell nuclei. These nuclei include open shell isotopes with the number of protons less than 20 and neutrons greater than 20, for which experimental data are available. Shell model calculations are performed with full $sd$ shell model space for $Z$\ensuremath{-}8
R. A. Radhi+2 more
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Local spin torque induced by electron electric dipole moment in the Ybf molecule
, 2014In this study, we show the modification of the equation of motion of the electronic spin, which is derived by the quantum electron spin vorticity principle, by the effect of the electron electric dipole moment (EDM).
M. Fukuda+3 more
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