O. N. Prudnikov

Systematic study of tunable laser cooling for trapped-ion experiments

A. P. Kulosa [1], O. N. Prudnikov [3,4], D. Vadlejch [1,2], H. A. Fürst, A. A. Kirpichnikova [3], A. V. Taichenachev [3,4], V. I. Yudin [3,4,5,1,2], T. E. Mehlstäubler

Abstract

We report on a comparative analysis of quenched sideband cooling in trapped ions. We introduce a theoretical approach for time-efficient simulation of the temporal cooling characteristics and derive the optimal conditions providing fast laser cooling into the ion's motional ground state. The simulations were experimentally benchmarked with a single $^{172}$Yb$^+$ ion confined in a linear Paul trap. Sideband cooling was carried out on a narrow quadrupole transition, enhanced with an additional clear-out laser for controlling the effective linewidth of the cooling transition. Quench cooling was thus for the first time studied in the resolved sideband, intermediate and semi-classical regime. We discuss the non-thermal distribution of Fock states during laser cooling and reveal its impact on time dilation shifts in optical atomic clocks.

Probe field ellipticity-induced shift in an atomic clock

V. I. Yudin [1,2,3], A. V. Taichenachev [1,2], O. N. Prudnikov [1,2], M. Yu. Basalaev [1,2,3,4,5], V. G. Pal'chikov, M. von Boehn [6,7], T. E. Mehlstäubler, S. N. Bagayev [1,2]

Abstract

We investigate the probe field induced shift for atomic lattice-based and ion-trap clocks, which can be considered as a near resonant ac-Stark shift, connected to the Zeeman structure of atomic levels and their splitting in a dc magnetic field. This shift arises from possible residual ellipticity in the polarization of the probe field and uncertainty in the magnetic field orientation. Such a shift can have an arbitrary sign and, for some experimental conditions, can reach the fractional value of the order of 10$^{-18}$-10$^{-19}$, i.e., it is not negligible. Thus, it should be taken into account in the uncertainty budgets for the modern ultra-precise atomic clocks. In addition, it is shown that when using hyper-Ramsey spectroscopy, this shift can be reduced to a level much lower than $10^{-19}$.