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

Physica A Statistical Mechanics and its Applications

Transferring squeezing and statistics in coupled circuits

Hilário Rodrigues, D. Portes, S. B. Duarte, B. Baseia

Published Aug 1, 2002• 5 citations
Publisher
DOI
10.1016/s0378-4371(02)00825-7

Related papers

Transference of squeezing in coupled oscillators

Cezar Augusto Bonato, B. Baseia

International Journal of Theoretical Physics•Jul 1, 1994•6 citations

Squeezing Effects of a Mesoscopic Dissipative Coupled Circuit

Yinghua Ji, Lei Min-Sheng

International Journal of Theoretical Physics•Jul 1, 2002•9 citations

Entangled State Evolution and Entanglement Transfer in Quantum Mesoscopic Coupled Circuits

Zhuoyuan Wang, Shi Yao Chong, Peihong Cheng +2 more

A mesoscopic circuit, where field quantization (e.g., coherent states and squeezed states) can be exhibited, is one of the ideal quantum systems for manifesting diverse quantum field theoretical phenomena and thermally statistical characteristics. Because of inevitable electromagnetic coupling (e.g., mutual capacitor coupling and mutual inductor coupling) in two neighboring mesoscopic electric circuits, quantum effects relevant to mesoscopic circuit coupling may play a key role in some devices of quantum information processing. Such a circuit coupling can lead to circuit entangled states, where the Fock number states of energy quanta in different circuits are entangled with each other. Since the time dependence in parameters of coupled-circuit Hamiltonian would result from environmental perturbations (e.g., temperature fluctuations in devices) or from some controllable manipulation (e.g., an incident ultrasonic wave), the circuit entangled states would evolve due to these external conditions. Time evolution of entangled states in coupled mesoscopic circuits is considered within a framework of time-dependent quantum theoretical formalism. Note that an applied photon field can also be coupled to such quantum entangled circuits. Then it is possible that an effect of entanglement transfer (i.e., transportation of superposition coefficients in the entangled state) from the quantum mesoscopic coupled LC circuits to the applied external photon field would also occur under some proper parameter conditions. The present characteristics of both quantized coupled mesoscopic circuits and entanglement transfer can also be found in some alternative microscopic- and mesoscopic-scale devices such as the systems in cavity quantum electrodynamics (QED).

Journal of the Physical Society of Japan•Aug 18, 2020•0 citations

Amplification of the coupling strength in a hybrid quantum system

Wei Xiong, Yueyin Qiu, Lian-Ao Wu +1 more

Realization of strong coupling between two different quantum systems is important for fast transferring quantum information between them, but its implementation is difficult in some hybrid quantum systems. Here we propose a scheme to enhance the coupling strength between a single nitrogen-vacancy center and a superconducting circuit via squeezing. The main recipe of our scheme is to construct a unitary squeezing transformation by directly tuning the specifically-designed superconducting circuit. Using the experimentally accessible parameters of the circuit, we find that the coupling strength can be largely amplified by applying the squeezing transformations to the system. This provides a new path to enhance the coupling strengths in hybrid quantum systems.

arXiv:1709.06433•New Journal of Physics•Apr 3, 2018•17 citations

An Introduction to Squeezed States

John R. Klauder

Springer eBooks•Jan 1, 1986•1 citation

Quantum-statistical property of optical diode based on cavity QED

Haozhen Li, Jingping Xu, Da‐Wei Wang +3 more

An optical diode made of an asymmetric cavity containing a two-level atom is investigated. We focus on the quantum-statistical property of the transmitted field with nonclassical light input. Both coherent and squeezed light inputs have been considered. The results show that the transmitted contrast of such optical diode is independent of the statistical properties of the incident light but is only sensitive to its intensity. On the other hand, the quantum-statistical property, i.e., the squeezing, of the transmitted field strongly depends on the statistical properties and directions of the incident light. For squeezed light input, the degree of the squeezing of the transmitted field can be remarkably enhanced. Moreover, the squeezing of the amplitude quadrature of the incident light can be transferred to the phase quadrature due to the coupling of the light and the atom.

Physical Review A•Jul 17, 2017•9 citations
A mesoscopic circuit, where field quantization (e.g., coherent states and squeezed states) can be exhibited, is one of the ideal quantum systems for manifesting diverse quantum field theoretical phenomena and thermally statistical characteristics. Because of inevitable electromagnetic coupling (e.g., mutual capacitor coupling and mutual inductor coupling) in two neighboring mesoscopic electric circuits, quantum effects relevant to mesoscopic circuit coupling may play a key role in some devices of quantum information processing. Such a circuit coupling can lead to circuit entangled states, where the Fock number states of energy quanta in different circuits are entangled with each other. Since the time dependence in parameters of coupled-circuit Hamiltonian would result from environmental perturbations (e.g., temperature fluctuations in devices) or from some controllable manipulation (e.g., an incident ultrasonic wave), the circuit entangled states would evolve due to these external conditions. Time evolution of entangled states in coupled mesoscopic circuits is considered within a framework of time-dependent quantum theoretical formalism. Note that an applied photon field can also be coupled to such quantum entangled circuits. Then it is possible that an effect of entanglement transfer (i.e., transportation of superposition coefficients in the entangled state) from the quantum mesoscopic coupled LC circuits to the applied external photon field would also occur under some proper parameter conditions. The present characteristics of both quantized coupled mesoscopic circuits and entanglement transfer can also be found in some alternative microscopic- and mesoscopic-scale devices such as the systems in cavity quantum electrodynamics (QED).
Realization of strong coupling between two different quantum systems is important for fast transferring quantum information between them, but its implementation is difficult in some hybrid quantum systems. Here we propose a scheme to enhance the coupling strength between a single nitrogen-vacancy center and a superconducting circuit via squeezing. The main recipe of our scheme is to construct a unitary squeezing transformation by directly tuning the specifically-designed superconducting circuit. Using the experimentally accessible parameters of the circuit, we find that the coupling strength can be largely amplified by applying the squeezing transformations to the system. This provides a new path to enhance the coupling strengths in hybrid quantum systems.
An optical diode made of an asymmetric cavity containing a two-level atom is investigated. We focus on the quantum-statistical property of the transmitted field with nonclassical light input. Both coherent and squeezed light inputs have been considered. The results show that the transmitted contrast of such optical diode is independent of the statistical properties of the incident light but is only sensitive to its intensity. On the other hand, the quantum-statistical property, i.e., the squeezing, of the transmitted field strongly depends on the statistical properties and directions of the incident light. For squeezed light input, the degree of the squeezing of the transmitted field can be remarkably enhanced. Moreover, the squeezing of the amplitude quadrature of the incident light can be transferred to the phase quadrature due to the coupling of the light and the atom.