Ping Zhang

Evaluation of blackbody radiation shift with temperature associated fractional uncertainty at 10E-18 level for 40Ca+ ion optical clock

Ping Zhang [1,2,3,4], Jian Cao [1,2], Hua-lin Shu [1,2], Jin-bo Yuan [1,2,3], Juan-juan Shang, Kai-feng Cui [1,2,3], Si-jia Chao [1,2,3], Shao-mao Wang [1,2,3], Dao-xin Liu [1,2,3], Xue-ren Huang [1,2]

Abstract

In this paper, blackbody radiation (BBR) temperature rise seen by the $^{40}$Ca$^+$ ion confined in a miniature Paul trap and its uncertainty have been evaluated via finite-element method (FEM) modelling. The FEM model was validated by comparing with thermal camera measurements, which were calibrated by PT1000 resistance thermometer, at several points on a dummy trap. The input modelling parameters were analyzed carefully in detail, and their contributions to the uncertainty of environment temperature were evaluated on the validated FEM model. The result shows that the temperature rise seen by $^{40}$Ca$^+$ ion is 1.72 K with an uncertainty of 0.46 K. It results in a contribution of 2.2 mHz to the systematic uncertainty of $^{40}$Ca$^+$ ion optical clock, corresponding to a fractional uncertainty 5.4$\times$10$^{-18}$. This is much smaller than the uncertainty caused by the BBR shift coefficient, which is evaluated to be 4.8 mHz and at 10$^{-17}$ level in fractional frequency units.

A transportable 40Ca+ single-ion clock with $7.7\times 10^{-17}$ systematic uncertainty

Jian Cao [1,2], Ping Zhang [1,2,3,4], Junjuan Shang [1,2,3], Kaifeng Cui [1,2,3], Jinbo Yuan [1,2,3], Sijia Chao [1,2,3], Shaomao Wang [1,2,3], Hualin Shu [1,2], Xueren Huang [1,2]

Abstract

A transportable optical clock refer to the $4s^2S_{1/2}-3d^2D_{5/2}$ electric quadrupole transition at 729 nm of single $^{40}Ca^+$ trapped in mini Paul trap has been developed. The physical system of $^{40}Ca^+$ optical clock is re-engineered from a bulky and complex setup to an integration of two subsystems: a compact single ion unit including ion trapping and detection modules, and a compact laser unit including laser sources, beam distributor and frequency reference modules. Apart from the electronics, the whole equipment has been constructed within a volume of 0.54 $m^3$. The systematic fractional uncertainty has been evaluated to be $7.7\times 10^{-17}$, and the Allan deviation fits to be $2.3\times {10}^{-14}/\sqrtτ$ by clock self-comparison with a probe pulse time 20 ms.