2022/10/26 by Dörscher, Sören, Klose, Joshua, Palli, Sarath Maratha +1 · 1 citation
#Atomic Physics (physics.atom-ph) #FOS: Physical sciences
paper · doi:10.48550/arxiv.2210.14727
To operate an optical lattice clock at a fractional uncertainty below 10-17, one must typically consider not only electric-dipole (E1) interaction between an atom and the lattice light field when characterizing the resulting lattice light shift of the clock transition but also higher-order multipole contributions, such as electric-quadrupole (E2) and magnetic-dipole (M1) interactions. However, strongly incompatible values have been reported for the E2-M1 polarizability difference of the clock states (5s5p) 3P0 and (5s2) 1S0 of strontium [Ushijima et al., Phys. Rev. Lett. 121 263202 (2018); Porsev et al., Phys. Rev. Lett. 120, 063204 (2018)]. This largely precludes operating strontium clocks with uncertainties of few 10-18, as the resulting lattice light shift corrections deviate by up to 1 × 10-17 from each other at typical trap depths. We have measured the E2-M1 polarizability difference using our 87Sr lattice clock and find a value of Δαqm = -987+174-223 μHz. This result is in very good agreement with the value reported by Ushijima et al.