Abstract
Abstract
We present a method for measuring the polarizability of Rydberg ions confined in the harmonic potential of a Paul trap. For a highly excited electronic state, the coupling between the electronic wave function and the trapping field modifies the excitation spectra depending on the motional state of the ion. This interaction strongly depends on the polarizability of the excited state and manifests itself in the state-dependent secular frequencies of the ion. We initialize a single trapped 40Ca+ ion from the motional ground state into coherent states with
|
α
|
up to 12 using electric voltages on the trap segments. The internal state, firstly initialised in the long-lived 3D
5
/
2
state, is excited to a Rydberg S
1
/
2
-state via the 5P
3
/
2
state in a two-photon process. We probe the depletion of the 3D
5
/
2
state owing to the Rydberg excitation followed by a decay into the internal ground 4S
1
/
2
state. By analysing the obtained spectra we extract the polarizability of Rydberg states which agree with numerical calculations. The method is applicable to different Rydberg states regardless of their principal or angular quantum numbers. An accurate value of the state polarizability is needed for quantum gate operations with Rydberg ion crystals.
Funder
the Deutsche Forschungsgemeinschaft (DFG) within the SPP 1929 Giant interactions in Rydberg Systems
the European Union’s Horizon 2020 research and innovation programme the Marie Sklodowska-Curie grant
the QuantERA grant ERyQSenS.
Subject
General Physics and Astronomy
Cited by
2 articles.
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