scholarly journals Coupling effects in single-mode and multimode resonator-coupled system

2019 ◽  
Vol 27 (13) ◽  
pp. 17718 ◽  
Author(s):  
Cuixiu Xiong ◽  
Hongjian Li ◽  
Hui Xu ◽  
Mingzhuo Zhao ◽  
Baihui Zhang ◽  
...  
1996 ◽  
Vol 125 (4-6) ◽  
pp. 369-376 ◽  
Author(s):  
Oscar G. Calderón ◽  
Isabel Gonzalo

2018 ◽  
Vol 16 (02) ◽  
pp. 1850017 ◽  
Author(s):  
Iskandar Bahari ◽  
Timothy P. Spiller ◽  
Shane Dooley ◽  
Anthony Hayes ◽  
Francis McCrossan

We extend the study of the Jayne–Cummings (JC) model involving a pair of identical two-level atoms (or qubits) interacting with a single mode quantized field. We investigate the effects of replacing the radiation field mode with a composite spin, comprising [Formula: see text] qubits, or spin-1/2 particles. This model is relevant for physical implementations in superconducting circuit QED, ion trap and molecular systems. For the case of the composite spin prepared in a spin coherent state, we demonstrate the similarities of this set-up to the qubits-field model in terms of the time evolution, attractor states and in particular the collapse and revival of the entanglement between the two qubits. We extend our analysis by taking into account an effect due to qubit imperfections. We consider a difference (or “mismatch”) in the dipole interaction strengths of the two qubits, for both the field mode and composite spin cases. To address decoherence due to this mismatch, we then average over this coupling strength difference with distributions of varying width. We demonstrate in both the field mode and the composite spin scenarios that increasing the width of the “error” distribution increases suppression of the coherent dynamics of the coupled system, including the collapse and revival of the entanglement between the qubits.


1992 ◽  
Vol 237 ◽  
pp. 57-71 ◽  
Author(s):  
Paola Cessi ◽  
W. R. Young

We study fixed-flux convection in a long, narrow slot which is inclined to the horizontal. (Gravity is in the vertical direction, and horizontal is perpendicular to this.) Because of the fixed-flux boundary conditions the convective modes have much larger lengthscales in the along-slot direction than in the transverse direction. In the case of a horizontal slot this disparity in scales has been previously exploited to obtain an amplitude equation for the single mode which first becomes unstable as the Rayleigh number is increased above critical. When the slot is tilted we show that there is a distinguished limit in which there are two active modes in the slightly supercritical regime. This new limit is when the horizontal wavenumber, the supercriticality, and the tilt of the slot away from vertical, are all small. A modification of the well-known expansion for fixed flux convection in a horizontal slot leads to a coupled system of partial differential equations for the amplitudes of the two modes.Numerical solution of this system suggests that all initial conditions eventually evolve into one of the two states, both of which consist of a single, steady roll in the cavity. The states are distinguished by the direction of circulation of the roll, and by the buoyancy fields, which are quite different in the two cases.


2017 ◽  
Vol 35 (9) ◽  
pp. 1710-1717 ◽  
Author(s):  
Qi Lu ◽  
Zhenzheng Wang ◽  
Qingzhong Huang ◽  
Wei Jiang ◽  
Zijin Wu ◽  
...  

2014 ◽  
Vol 23 (04) ◽  
pp. 1450052
Author(s):  
S. S. Hassan ◽  
R. A. Alharbey ◽  
H. Al-Zaki

Exact analytical results are derived for the coupled system of nondissipative single mode quantized harmonic oscillator (HO) and arbitrary pulse shape. Specifically, for a sin2-pulse shape, the transient fluorescent spectrum is obtained in the general case of initial coherent state |α〉 of the HO. The dominant central Lorentzian is surrounded by weak oscillations due to the larger number of sequential pulses which get amplified asymmetrically in the nonresonant case as a result of balancing and interference processes between the initial excitation (|α2|) and the strength of the exciting pulse. Further pronounced oscillations is noticed with "hole burning" structure in the central peak due to nonzero phase of the initial amplitude (α).


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