2019
DOI: 10.1038/s41467-019-09706-9
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Inner-shell clock transition in atomic thulium with a small blackbody radiation shift

Abstract: One of the key systematic effects limiting the performance of state-of-the-art optical clocks is the blackbody radiation (BBR) shift. Here, we demonstrate unusually low sensitivity of a 1.14 μm inner-shell clock transition in neutral Tm atoms to BBR. By direct polarizability measurements, we infer a differential polarizability of the clock levels of −0.063(30) atomic units corresponding to a fractional frequency BBR shift of only 2.3(1.1) × 10 −18 at room temperature. This amount is seve… Show more

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Cited by 89 publications
(45 citation statements)
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“…While we demonstrate the coherent suppression for a simple single-ion optical atomic clock system, we see wide application in high-precision spectroscopy and other clock systems [22][23][24][25][26]. The method may be particularly beneficial for optical clocks based on ions in Coulomb crystals [24,25].…”
mentioning
confidence: 88%
“…While we demonstrate the coherent suppression for a simple single-ion optical atomic clock system, we see wide application in high-precision spectroscopy and other clock systems [22][23][24][25][26]. The method may be particularly beneficial for optical clocks based on ions in Coulomb crystals [24,25].…”
mentioning
confidence: 88%
“…Unlike most ultracold atoms, many lanthanides exhibit fine structure splitting even in their ground state. A recent example, attracting much attention for its application to quantum metrology, is the near infra-red innershell clock transition in Thulium (Tm), which connects two fine-structure levels (J = 7/2 → J = 5/2) of the electronic ground-state [11].…”
Section: Complex Energy Spectrummentioning
confidence: 99%
“…Since most atomic metals used today for laser cooling and trapping have a low saturation pressure at room temperature, a typical atomic source consists of an effusive thermal atomic beam, which is extracted from a high temperature oven. Some examples of cold atoms produced from oven source include atomic species like alkaline-earth metals (Mg 1 , Ca 2 , Sr 3 , 4 , Ba 5 , Ra 6 ), lanthanides (Eu 7 , 8 , Dy 9 , Ho 10 , Er 11 , Tm 12 , Yb 13 ), and transition-metals (Cr 14 , 15 ). Due to the high longitudinal velocity of the hot atomic beam, a Zeeman slower is often required between the oven and the final magneto-optical trap (MOT).…”
Section: Introductionmentioning
confidence: 99%