Inversions of qubit energy levels in deep-strongly-coupled qubit-oscillator circuits
ORAL
Abstract
The electromagnetic field inside a cavity renormalizes the transition frequency of an atom inside the cavity. The Lamb (n = 0) and n-photon ac-Stark shifts can be written as Δ - Δn, where Δ and Δn are respectively the transition frequencies of a non-interacting and renormalized atom. In the limit of Δ « ω, where ω is the resonance frequency of the cavity, Δn can be written as [1] Δn/Δ = exp[-2(g/ω)2]Ln[(2g/ω)2], where g is the coupling constant between the atom and the electromagnetic field in the cavity and Ln is a Laguerre polynomial. This equation indicates that Δn changes sign when Ln crosses zero; the atom's ground and excited states are “inverted”. We use circuits of a flux qubit deep-strongly coupled to an LC oscillator [2], where g ≈ ω. The experimentally observed qubit frequencies Δn (n = 0, 1, 2) were very close to those given by the equation above. [1] S. Ashhab and F. Nori, PRA 81, 052311 (2010). [2] F. Yoshihara, T. Fuse et al., Nat. Phys. 13, 44 (2017).
*This work was supported by the Scientific Research (S) Grant No. JP25220601 by the Japanese Society for the Promotion of Science (JSPS), and the Japan Science and Technology Agency’s (JST) CREST program entitled "Creation of an innovative quantum technology platform based on the advanced control of quant
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Presenters
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Fumiki Yoshihara
- Advanced ICT Institute, National Institute of Information and Communications Technology