Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Bulletin of the American Physical Society

Circuit QED without selection rules: the dispersive regime of the fluxonium qubit

Guanyu Zhu, Jens Koch

Published Mar 23, 2011• 0 citations
OpenAlex

Related papers

Readout of fluxonium qubits in circuit QED

Konstantin Nesterov, Long B. Nguyen, Aaron Somoroff +7 more

Bulletin of the American Physical Society•Mar 2, 2020•0 citations

Second order dispersive regime of circuit QED with a transmon qubit

Maxime Boissonneault, Jay Gambetta, Alexandre Blais

Bulletin of the American Physical Society•Mar 19, 2009•0 citations

Dynamics of dispersive single qubit read-out in circuit QED

R. Bianchetti, Stefan Filipp, Alexandre Blais +1 more

Bulletin of the American Physical Society•Mar 19, 2009•0 citations

Circuit QED with fluxonium qubits: Theory of the dispersive regime

Guanyu Zhu, David Ferguson, Vladimir Manucharyan +1 more

In circuit QED, protocols for quantum gates and readout of superconducting qubits often rely on the dispersive regime, reached when the qubit-photon detuning $\ensuremath{\Delta}$ is large compared to the mutual coupling strength. For qubits including the Cooper-pair box and transmon, selection rules dramatically restrict the contributions to dispersive level shifts $\ensuremath{\chi}$. By contrast, in the absence of selection rules many virtual transitions contribute to $\ensuremath{\chi}$ and can produce sizable dispersive shifts even at large detuning. We present theory for a generic multilevel qudit capacitively coupled to one or multiple harmonic modes and give general expressions for the effective Hamiltonian in second- and fourth-order perturbation theory. Applying our results to the fluxonium system, we show that the absence of strong selection rules explains the surprisingly large dispersive shifts observed in experiments and leads to the prediction of a two-photon vacuum Rabi splitting. Quantitative predictions from our theory are in good agreement with experimental data over a wide range of magnetic flux and reveal that fourth-order resonances are important for the phase modulation observed in fluxonium spectroscopy.

arXiv:1210.1605•Physical Review B•Jan 14, 2013•134 citations

Asymptotic expressions for charge-matrix elements of the fluxonium circuit

Guanyu Zhu, Jens Koch

In charge-coupled circuit QED systems, transition amplitudes and dispersive shifts are governed by the matrix elements of the charge operator. For the fluxonium circuit, these matrix elements are not limited to nearest-neighbor energy levels and are conveniently tunable by magnetic flux. Previously, their values were largely obtained numerically. Here, we present analytical expressions for the fluxonium charge matrix elements. We show that new selection rules emerge in the asymptotic limit of large Josephson energy and small inductive energy. We illustrate the usefulness of our expressions for the qualitative understanding of charge matrix elements in the parameter regime probed by previous experiments.

arXiv:1305.3965•Physical Review B•Apr 29, 2013•14 citations

Circuit QED with phase-biased qubits

Jérôme Bourassa, Alexandre Blais, Michel Devoret +1 more

Bulletin of the American Physical Society•Mar 12, 2008•0 citations
In circuit QED, protocols for quantum gates and readout of superconducting qubits often rely on the dispersive regime, reached when the qubit-photon detuning $\ensuremath{\Delta}$ is large compared to the mutual coupling strength. For qubits including the Cooper-pair box and transmon, selection rules dramatically restrict the contributions to dispersive level shifts $\ensuremath{\chi}$. By contrast, in the absence of selection rules many virtual transitions contribute to $\ensuremath{\chi}$ and can produce sizable dispersive shifts even at large detuning. We present theory for a generic multilevel qudit capacitively coupled to one or multiple harmonic modes and give general expressions for the effective Hamiltonian in second- and fourth-order perturbation theory. Applying our results to the fluxonium system, we show that the absence of strong selection rules explains the surprisingly large dispersive shifts observed in experiments and leads to the prediction of a two-photon vacuum Rabi splitting. Quantitative predictions from our theory are in good agreement with experimental data over a wide range of magnetic flux and reveal that fourth-order resonances are important for the phase modulation observed in fluxonium spectroscopy.
In charge-coupled circuit QED systems, transition amplitudes and dispersive shifts are governed by the matrix elements of the charge operator. For the fluxonium circuit, these matrix elements are not limited to nearest-neighbor energy levels and are conveniently tunable by magnetic flux. Previously, their values were largely obtained numerically. Here, we present analytical expressions for the fluxonium charge matrix elements. We show that new selection rules emerge in the asymptotic limit of large Josephson energy and small inductive energy. We illustrate the usefulness of our expressions for the qualitative understanding of charge matrix elements in the parameter regime probed by previous experiments.