Evolution of a hybrid micro–macro entangled state of the qubit–oscillator system via the generalized rotating wave approximation. (17th March 2016)

• Record Type: Journal Article
• Authors: Chakrabarti, R; Yogesh, V
• Is Part Of: Journal of physics. Volume 49:Number 7(2016:Apr. 01)
• Publication Date: 2016-03-17
• Subjects: qubit–oscillator interacting system -- generalized rotating wave approximation -- hybrid entangled states -- phase space quasi probabilities -- kitten states and multiple time scales -- squeezed states; Atoms -- Periodicals; Molecules -- Periodicals; Optics -- Periodicals; Nuclear physics -- Periodicals; 539.6
• DOI: 10.1088/0953-4075/49/7/075502
• Languages: English
• ISSNs: 0953-4075

Abstract

Abstract: We study the evolution of the hybrid entangled states in a bipartite (ultra) strongly coupled qubit-oscillator system. Using the generalized rotating wave approximation the reduced density matrices of the qubit and the oscillator are obtained. The reduced density matrix of the oscillator yields the phase space quasi probability distributions such as the diagonal P -representation, the Wigner W -distribution and the Husimi Q -function. In the strong coupling regime the Q -function evolves to uniformly separated macroscopically distinct Gaussian peaks representing 'kitten' states at certain specified times that depend on multiple time scales present in the interacting system. The ultrastrong coupling strength of the interaction triggers appearance of a large number of modes that quickly develop a randomization of their phase relationships. A stochastic averaging of the dynamical quantities sets in, and leads to the decoherence of the system. The delocalization in the phase space of the oscillator is studied by using the Wehrl entropy. The negativity of the W -distribution reflects the departure of the oscillator from the classical states, and allows us to study the underlying differences between various information-theoretic measures such as the Wehrl entropy and the Wigner entropy. Other features of nonclassicality such as the existence of the squeezed states and appearance of negative values of the Mandel parameter are realized during the course of evolution of the bipartite system. In the parametric regime studied here these properties do not survive in the time-averaged limit.