Crossover from weak to strong coupling regime in dispersive circuit QED
arXiv:cond-mat/0606734 · doi:10.1209/0295-5075/80/40011
Abstract
We study the decoherence of a superconducting qubit due to the dispersive coupling to a damped harmonic oscillator. We go beyond the weak qubit-oscillator coupling, which we associate with a phase Purcell effect, and enter into a strong coupling regime, with qualitatively different behavior of the dephasing rate. We identify and give a physicaly intuitive discussion of both decoherence mechanisms. Our results can be applied, with small adaptations, to a large variety of other physical systems, e. g. trapped ions and cavity QED, boosting theoretical and experimental decoherence studies.
Published version
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Cited by in corpus (8)
- Photon Shot Noise Dephasing in the Strong-Dispersive Limit of Circuit QED
- Circuit QED with fluxonium qubits: theory of the dispersive regime
- Probing the quantum coherence of a nanomechanical resonator using a superconducting qubit: I. Echo scheme
- Theory of Josephson Photomultipliers: Optimal Working Conditions and Back Action
- Stochastic Wave-Function Unravelling of the Generalized Lindblad Master Equation
- Photon-noise-tolerant dispersive readout of a superconducting qubit using a nonlinear Purcell filter
- Relaxation of a qubit measured by a driven Duffing oscillator
- Vacuum-fluctuation-induced Dephasing of a Qubit in Circuit Quantum Electrodynamics