Magic intensity trapping of the Mg lattice clock with light shift suppressed below
arXiv:1909.07692 · doi:10.1103/PhysRevA.101.053414
Abstract
Progress in atomic optical clocks with total uncertainty of or below requires a precise estimation of multipolar and higher-order effects due to atom-field interactions. Magnesium is an attractive candidate for optical lattice clocks because it is insensitive to blackbody radiation and has a large quality factor. We employ a combined method of the Dirac-Fock plus core polarization and the relativistic configuration interaction to calculate the dynamic multipolar polarizabilities and the hyperpolarizabilities of the atomic Mg clock. The lattice light shift against variation of the laser detuning and trap depth is also investigated. We find that there exists a distinctive operational magic lattice intensity of ( is the lattice photon recoil energy) that reduces the total light shift below over 14\% of the trap depth variation, which will pave the way for the development of a new time-frequency standard of the Mg lattice clock.
6 pages, 1 figures
References in corpus (11)
- Systematic evaluation of an atomic clock at 2e-18 total uncertainty
- An Al quantum-logic clock with systematic uncertainty below
- Frequency ratio of two optical clock transitions in Yb and constraints on the time-variation of fundamental constants
- Improved limit on a temporal variation of from comparisons of Yb and Cs atomic clocks
- High accuracy correction of blackbody radiation shift in an optical lattice clock
- Operational Magic Intensity for Sr Optical Lattice Clocks
- Hyperpolarizability and operational magic wavelength in an optical lattice clock
- Strategies for reducing the light shift in atomic clocks
- Coherence preservation of a single neutral atom qubit transferred between magic-intensity optical traps
- Optical Lattice Polarization Effects on Hyperpolarizability of Atomic Clock Transitions
- High-precision nonadiabatic calculations of dynamic polarizabilities and hyperpolarizabilities for the lowlying vibrational-rotational states of hydrogen molecular ions