Bandyopadhyay Biswabibek, Khatun Taniya, Biswas Debabrata, Banerjee Tanmoy
Chaos and Complex Systems Research Laboratory, Department of Physics, University of Burdwan, Burdwan 713 104, West Bengal, India.
Department of Physics, Bankura University, Bankura 722 155, West Bengal, India.
Phys Rev E. 2020 Dec;102(6-1):062205. doi: 10.1103/PhysRevE.102.062205.
We study the quantum manifestations of homogeneous and inhomogeneous oscillation suppression states in coupled identical quantum oscillators. We consider quantum van der Pol oscillators coupled via weighted mean-field diffusive coupling and, using the formalism of open quantum systems, we show that, depending on the coupling and the density of mean-field, two types of quantum amplitude death occurs, namely, squeezed and nonsqueezed quantum amplitude death. Surprisingly, we find that the inhomogeneous oscillation suppression state (or the oscillation death state) does not occur in the quantum oscillators in the classical limit. However, in the deep quantum regime we discover an oscillation death-like state which is manifested in the phase space through the symmetry-breaking bifurcation of the Wigner function. Our results also hint toward the possibility of the transition from quantum amplitude death to oscillation death state through the "quantum" Turing-type bifurcation. We believe that the observation of quantum oscillation death state will deepen our knowledge of symmetry-breaking dynamics in the quantum domain.
我们研究了耦合相同量子振子中均匀和非均匀振荡抑制态的量子表现。我们考虑通过加权平均场扩散耦合的量子范德波尔振子,并使用开放量子系统的形式体系表明,根据耦合和平均场密度的不同,会出现两种类型的量子振幅死亡,即压缩和非压缩量子振幅死亡。令人惊讶的是,我们发现在经典极限下量子振子中不会出现非均匀振荡抑制态(或振荡死亡态)。然而,在深度量子区域,我们发现了一种类似振荡死亡的状态,它通过维格纳函数的对称性破缺分岔在相空间中表现出来。我们的结果还暗示了通过“量子”图灵型分岔从量子振幅死亡转变为振荡死亡态的可能性。我们相信,对量子振荡死亡态的观测将加深我们对量子领域中对称性破缺动力学的认识。