The atomic electric dipole moment induced by the nuclear electric dipole moment; the magnetic moment effect
arXiv:1012.0627 · doi:10.1103/PhysRevA.83.042507
Abstract
We have considered a mechanism for inducing a time-reversal violating electric dipole moment (EDM) in atoms through the interaction of a nuclear EDM (d_N) with the hyperfine interaction, the "magnetic moment effect". We have derived the operator for this interaction and presented analytical formulas for the matrix elements between atomic states. Induced EDMs in the diamagnetic atoms 129Xe, 171Yb, 199Hg, 211Rn, and 225Ra have been calculated numerically. From the experimental limits on the atomic EDMs of 129Xe and 199Hg, we have placed the following constraints on the nuclear EDMs, |d_N(129Xe)|< 1.1 * 10^{-21} |e|cm and |d_N(199Hg)|< 2.8 * 10^{-24} |e|cm.
8 pages 1) Some typos are corrected. 2) A comparison of contributions to the atomic EDM due to the nuclear EDM and the nuclear Schiff moment is added
References in corpus (6)
- Improved limit on the permanent electric dipole moment of 199Hg
- Resonance method of electric-dipole-moment measurements in storage rings
- Fully self-consistent calculations of nuclear Schiff moments
- Calculation of P,T-odd electric dipole moments for diamagnetic atoms Xe, Yb, Hg, Rn, and Ra
- Atomic electric dipole moments of He and Yb induced by nuclear Schiff moments
- Schiff Theorem Revisited
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- Observation of the nuclear magnetic octupole moment of Yb from precise measurements of hyperfine structure in the state
- Shielding of an external oscillating electric field inside atoms
- Enhanced nuclear Schiff and electric dipole moments in nuclei with an octupole deformation
- Electric field on nucleus due to phonon lattice oscillations in solid states