| Literature DB >> 36198794 |
Qi Shen1,2,3, Jian-Yu Guan1,2,3, Ji-Gang Ren1,2,3, Ting Zeng1,2,3, Lei Hou1,2,3, Min Li1,2,3, Yuan Cao1,2,3, Jin-Jian Han1,2,3, Meng-Zhe Lian1,2,3, Yan-Wei Chen1,2,3, Xin-Xin Peng1,2,3, Shao-Mao Wang1,2,3, Dan-Yang Zhu1,2,3, Xi-Ping Shi4, Zheng-Guo Wang1,2,3, Ye Li4, Wei-Yue Liu4, Ge-Sheng Pan1,2,3, Yong Wang5, Zhao-Hui Li6, Jin-Cai Wu3,6, Yan-Yan Zhang7, Fa-Xi Chen8, Chao-Yang Lu1,2,3, Sheng-Kai Liao1,2,3, Juan Yin1,2,3, Jian-Jun Jia3,6, Cheng-Zhi Peng1,2,3, Hai-Feng Jiang9,10,11, Qiang Zhang12,13,14,15,16, Jian-Wei Pan17,18,19.
Abstract
Networks of optical clocks find applications in precise navigation1,2, in efforts to redefine the fundamental unit of the 'second'3-6 and in gravitational tests7. As the frequency instability for state-of-the-art optical clocks has reached the 10-19 level8,9, the vision of a global-scale optical network that achieves comparable performances requires the dissemination of time and frequency over a long-distance free-space link with a similar instability of 10-19. However, previous attempts at free-space dissemination of time and frequency at high precision did not extend beyond dozens of kilometres10,11. Here we report time-frequency dissemination with an offset of 6.3 × 10-20 ± 3.4 × 10-19 and an instability of less than 4 × 10-19 at 10,000 s through a free-space link of 113 km. Key technologies essential to this achievement include the deployment of high-power frequency combs, high-stability and high-efficiency optical transceiver systems and efficient linear optical sampling. We observe that the stability we have reached is retained for channel losses up to 89 dB. The technique we report can not only be directly used in ground-based applications, but could also lay the groundwork for future satellite time-frequency dissemination.Entities:
Year: 2022 PMID: 36198794 DOI: 10.1038/s41586-022-05228-5
Source DB: PubMed Journal: Nature ISSN: 0028-0836 Impact factor: 69.504