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

Geometric phases and noise in circuit QED

Simon Jacques Berger

Published Jan 1, 2015• 0 citations
Publisher
DOI
10.3929/ethz-a-010460932

Related papers

Detecting non-Abelian geometric phase in circuit QED

Man-Lv Peng, Jian Zhou, Zheng‐Yuan Xue

arXiv:1303.0495•Quantum Information Processing•Mar 12, 2013•0 citations

Exploring the Effect of Noise on the Berry Phase using circuit QED

S. Berger, Marek Pechal, A. A. Abdumalikov +5 more

Bulletin of the American Physical Society•Mar 4, 2014•0 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

Unconventional Geometric Quantum Gate in Circuit QED

Zheng Xiao-Hu, Jun Dong, Yuwen Liu +2 more

We propose a scheme to implement an unconventional geometric phase gate in circuit QED, i.e. two superconducting charge qubits inside a superconducting transmission line resonator. The quantum operation depends only on global geometric features, and thus is insensitive to the state of the cavity mode.

Chinese Physics Letters•Jul 1, 2010•0 citations

Ultrafast quantum computation in ultrastrongly coupled circuit QED systems

Yimin Wang, Chu Guo, Guo-Qiang Zhang +2 more

The latest technological progress of achieving the ultrastrong-coupling regime in circuit quantum electrodynamics (QED) systems has greatly promoted the developments of quantum physics, where novel quantum optics phenomena and potential computational benefits have been predicted. Here, we propose a scheme to accelerate the nontrivial two-qubit phase gate in a circuit QED system, where superconducting flux qubits are ultrastrongly coupled to a transmission line resonator (TLR), and two more TLRs are coupled to the ultrastrongly-coupled system for assistant. The nontrivial unconventional geometric phase gate between the two flux qubits is achieved based on close-loop displacements of the three-mode intracavity fields. Moreover, as there are three resonators contributing to the phase accumulation, the requirement of the coupling strength to realize the two-qubit gate can be reduced. Further reduction in the coupling strength to achieve a specific controlled-phase gate can be realized by adding more auxiliary resonators to the ultrastrongly-coupled system through superconducting quantum interference devices. We also present a study of our scheme with realistic parameters considering imperfect controls and noisy environment. Our scheme possesses the merits of ultrafastness and noise-tolerance due to the advantages of geometric phases.

Scientific Reports•Mar 10, 2017•32 citations

Noise in quantum devices

E. S. R. Gopal

IEE-IERE Proceedings - India•Jan 1, 1972•0 citations
The latest technological progress of achieving the ultrastrong-coupling regime in circuit quantum electrodynamics (QED) systems has greatly promoted the developments of quantum physics, where novel quantum optics phenomena and potential computational benefits have been predicted. Here, we propose a scheme to accelerate the nontrivial two-qubit phase gate in a circuit QED system, where superconducting flux qubits are ultrastrongly coupled to a transmission line resonator (TLR), and two more TLRs are coupled to the ultrastrongly-coupled system for assistant. The nontrivial unconventional geometric phase gate between the two flux qubits is achieved based on close-loop displacements of the three-mode intracavity fields. Moreover, as there are three resonators contributing to the phase accumulation, the requirement of the coupling strength to realize the two-qubit gate can be reduced. Further reduction in the coupling strength to achieve a specific controlled-phase gate can be realized by adding more auxiliary resonators to the ultrastrongly-coupled system through superconducting quantum interference devices. We also present a study of our scheme with realistic parameters considering imperfect controls and noisy environment. Our scheme possesses the merits of ultrafastness and noise-tolerance due to the advantages of geometric phases.