2022
DOI: 10.1103/prxquantum.3.020326
|View full text |Cite|
|
Sign up to set email alerts
|

Controlling Rydberg Excitations Using Ion-Core Transitions in Alkaline-Earth Atom-Tweezer Arrays

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
2
1

Citation Types

1
11
0

Year Published

2022
2022
2023
2023

Publication Types

Select...
5
2

Relationship

1
6

Authors

Journals

citations
Cited by 26 publications
(14 citation statements)
references
References 41 publications
1
11
0
Order By: Relevance
“…From fits of the measured excitation energies to Eq. 1 we get the quantum defects δ 0,0 = 4.2721 (25) and δ 1,1 = 3.9535 (9), where the value for the 6sns 1 S 0 series is again in good agreement with Ref. [21].…”
Section: Statesupporting
confidence: 82%
See 1 more Smart Citation
“…From fits of the measured excitation energies to Eq. 1 we get the quantum defects δ 0,0 = 4.2721 (25) and δ 1,1 = 3.9535 (9), where the value for the 6sns 1 S 0 series is again in good agreement with Ref. [21].…”
Section: Statesupporting
confidence: 82%
“…For example, for Rydberg states with low angular momentum so-called isolated-core excitation, of the second electron can lead to auto-ionization of the Rydberg electron. This phenomenon can be used to control Rydberg excitations [8,9] or directly image Rydberg atoms without the need to apply high-voltage pulses [10,11]. Another attractive application is trapping of Rydberg atoms [12].…”
Section: Introductionmentioning
confidence: 99%
“…It can be suppressed by increasing Ω (up to the limit imposed by V r r ), but in practice, Ω is often constrained by the available laser power. We note that the Yb 3 S 1 series has similar interaction strength 28 , 38 and lifetime 32 to Rydberg series in alkali atoms.…”
Section: Resultsmentioning
confidence: 67%
“…This transition is highly cyclic, with a branching ratio of ≈1 × 10 −7 back into Q 41 . Population remaining in Rydberg states at the end of a gate can be converted into Yb + ions by autoionization on the 6 s → 6 p 1/2 Yb + transition at 369 nm 38 . The resulting slow-moving Yb + ions can be detected using fluorescence on the same Yb + transition, as has been previously demonstrated for ensembles of Sr + ions in ultracold strontium gases 42 (subspace B in Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Advances in optical trapping with tweezers [43][44][45][46][47] and ground state cooling [48][49][50] provide both a freely programmable geometric arrangement [51,52], including coherent transport of atoms [53], as well as scalability to hundreds of particles [54,55]. Experiments with circular Rydberg states [56][57][58] promise longer single particle lifetimes [59], with a future potential for scaling to even larger system sizes [60,61]. We note, however, that up until now Rydberg platforms have mainly focused on quantum simulation of spin-1/2 systems.…”
Section: Introductionmentioning
confidence: 99%