2022
DOI: 10.1038/s41586-022-05245-4
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An optical atomic clock based on a highly charged ion

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Cited by 52 publications
(34 citation statements)
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“…Several laser spectroscopic methods for forbidden transitions of trapped HCIs free from systematic Doppler shifts have been reported 46,64 . These demonstrations employed a simple fine-structure transition 2 P 1/2 -2 P 3/2 in the doublet ground term of Ar 13+ , whose transition energy is precisely known from direct wavelength measurements using passive spectroscopy 65,66 , leading to recent quantum logic spectroscopy 36,37 . However, many potential candidates for the HCI atomic clock are not directly accessible using such passive spectroscopy because they possess complicated level structures with hyperfine splitting, and their clock transitions do not emit in plasmas owing to their long lifetime.…”
Section: Discussionmentioning
confidence: 99%
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“…Several laser spectroscopic methods for forbidden transitions of trapped HCIs free from systematic Doppler shifts have been reported 46,64 . These demonstrations employed a simple fine-structure transition 2 P 1/2 -2 P 3/2 in the doublet ground term of Ar 13+ , whose transition energy is precisely known from direct wavelength measurements using passive spectroscopy 65,66 , leading to recent quantum logic spectroscopy 36,37 . However, many potential candidates for the HCI atomic clock are not directly accessible using such passive spectroscopy because they possess complicated level structures with hyperfine splitting, and their clock transitions do not emit in plasmas owing to their long lifetime.…”
Section: Discussionmentioning
confidence: 99%
“…A number of candidates for HCI clocks have been proposed [16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31] , and their transition wavelengths have been experimentally investigated [32][33][34][35] . Micke et al recently demonstrated quantum logic spectroscopy of HCIs using Ar 13+ , which has no hyperfine structure, promising realization of the HCI clocks 36,37 . For further HCI atomic clock development employing fascinated transitions highly sensitive to the α variation 15 , it is necessary to gain a better understanding of hyperfine structure in many-electron heavy HCIs with a nuclear spin.…”
mentioning
confidence: 99%
“…The first term in (10), which can also be written as p´a{4q f 0 , is due to correlations between the noise during the B and R interrogations of the same cycle, while the second term is due to correlations between one cycle and all the subsequent ones. For g " 1, only the first term in the sum over m is nonzero, but also for smaller gains, the sum converges after only a few terms.…”
Section: Noise-induced Servo Errormentioning
confidence: 99%
“…For the higher-order Thue-Morse sequence RBBR-BRRB, used, e.g., in [21], the first term in (10) More complex probing sequences can be treated similarly.…”
Section: Noise-induced Servo Errormentioning
confidence: 99%
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