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Dipole and solenoidal magnetic moments of electronic surface currents on toroidal nanostructures

Journal of Computer-Aided Materials Design, 2007
The 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
openaire   +2 more sources

Theory of electron density in a collisionless plasma in the vicinity of a magnetic dipole

Physics of Plasmas, 2018
This 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
semanticscholar   +1 more source

Electronic properties of CuS: Experimental determination of the magnetic hyperfine interactions and permanent electric dipole moment

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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Effects of electric dipole, anapole, and neutral weak magnetic moments of a proton in the polarized electron-proton electroweak scattering

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
openaire   +2 more sources

Transition-Dipole Moments for Electronic Excitations in Strong Magnetic Fields Using Equation-of-Motion and Linear Response Coupled-Cluster Theory

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
openaire   +3 more sources

The permanent dipole moment of TiN and the nuclear magnetic hyperfine structure in its X 2Σ+ and A 2Π electronic states

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
openaire   +2 more sources

Ab initio study of the electric dipole transition moment for the C̃←X̃ electronic transition in acetylene: theoretical predictions of the absorption and magnetic circular dichroism intensities

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 (CC), 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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Relativistic effects in many electron hyperfine structure III. Relativistic dipole and quadrupole interaction in europium and remeasurement of the nuclear magnetic dipole moments of151Eu and153Eu

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
openaire   +2 more sources

Magnetic dipole moments, electric quadrupole moments, and electron scattering form factors of neutron-rich sdpf cross-shell nuclei

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
openaire   +2 more sources

Local spin torque induced by electron electric dipole moment in the Ybf molecule

, 2014
In 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
semanticscholar   +1 more source

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