aiqbench analysis
This study demonstrates a critical milestone in hybrid quantum systems by achieving strong coupling between Rydberg helium atoms and a superconducting microwave resonator via AC Stark shifting. The successful observation of single-photon Rabi frequencies indicates progress toward scalable interfaces that could link neutral-atom qubits with fixed-frequency superconducting circuits for distributed quantum networks.
Interfacing Rydberg atoms with a chip-based superconducting microwave resonator using an ac-Stark-shifted single-photon transition
arXiv:2508.20292v2 Announce Type: replace-cross Abstract: Helium atoms in the 1s50s$\,^3$S$_1$ Rydberg level have been resonantly coupled to the $2\pi\times11.722$ GHz second harmonic mode of a chip-based superconducting coplanar waveguide microwave resonator. To achieve this, the single-photon electric-dipole-allowed 1s50s$\,^3$S$_1\rightarrow$ 1s50p$\,^3$P$_J$ transition was tuned into resonance with the resonator mode through the AC Stark shift induced by a second strong $2\pi\times3.350$ GHz microwave dressing field. The effects of this dressing field, and residual uncanceled DC electric fields at the location of the atoms close to the superconducting chip surface were interpreted with support from Floquet calculations of the energy level structure of the Rydberg states. To observe appreciable population transfer in the $1~\mu$s atom-resonator interaction time using this transition, which had an electric dipole moment of $1500\,e\,a_0$, pulsed microwave fields were injected into the resonator. From the photon occupation number in the resonator mode under these conditions, the single-photon Rabi frequency associated with the coupling of the atoms to the resonator was estimated to be $\sim2\pi\times100$ Hz. These results represent an important step toward operation of this Rydberg-atom-superconducting-circuit interface in the single-photon strong coupling regime.
Abstract:Helium atoms in the 1s50s$\,^3$S$_1$ Rydberg level have been resonantly coupled to the $2\pi\times11.722$ GHz second harmonic mode of a chip-based superconducting coplanar waveguide microwave resonator. To achieve this, the single-photon electric-dipole-allowed 1s50s$\,^3$S$_1\rightarrow$ 1s50p$\,^3$P$_J$ transition was tuned into resonance with the resonator mode through the AC Stark shift induced by a second strong $2\pi\times3.350$ GHz microwave dressing field. The effects of this dressing field, and residual uncanceled DC electric fields at the location of the atoms close to the superconducting chip surface were interpreted with support from Floquet calculations of the energy level structure of the Rydberg states. To observe appreciable population transfer in the $1~\mu$s atom-resonator interaction time using this transition, which had an electric dipole moment of $1500\,e\,a_0$, pulsed microwave fields were injected into the resonator. From the photon occupation number in the resonator mode under these conditions, the single-photon Rabi frequency associated with the coupling of the atoms to the resonator was estimated to be $\sim2\pi\times100$ Hz. These results represent an important step toward operation of this Rydberg-atom-superconducting-circuit interface in the single-photon strong coupling regime.
Atomic Physics (physics.atom-ph); Quantum Physics (quant-ph)
arXiv:2508.20292 [physics.atom-ph]
(or arXiv:2508.20292v2 [physics.atom-ph] for this version)
https://doi.org/10.48550/arXiv.2508.20292 Focus to learn more arXiv-issued DOI via DataCite
Phys. Rev. A 113, 013709 (2026)
https://doi.org/10.1103/hzd4-1x22 Focus to learn more DOI(s) linking to related resources
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Full text under the publisher's open licence · 289 words
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