Entanglement of two superconducting qubits induced by a thermal noise of a cavity with Kerr medium taking into account the atomic coherence

E. K. Bashkirov
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引用次数: 1

Abstract

The system consisting of two identical artificial atoms (qubits), resonantly interacting with the mode of quantum field of an ideal microwave cavity in the presence of Kerr nonlinearity, is considered. For the considered model, an exact solution of the quantum Liouville equation for the full density matrix of the system two qubits + resonator field mode is obtained. To solve the quantum equation of evolution, the representation of dressed states, that is, the eigenfunctions of the Hamiltonian, was used. A complete set of dressed states of the considered model is found. With its help, the solution of the evolution equation was initially found for coherent initial states of qubits and Fock states of the field, that is, states with a certain number of photons in the resonator mode. Then, the above solution was generalized to the case of the thermal state of the resonator field. A reduced density matrix of two qubits is found by averaging over the field variables. The two-qubit density matrix is used to calculate the parameter of qubit entanglement in the analytical form. Concurrence was chosen as a quantitative criterion for qubit entanglement. A numerical simulation of the time dependence of the consistency of qubits for various parameters of the model and the initial states of qubits was carried out. The most interesting result seems to be that taking into account the initial coherence of qubits in the model with Kerr nonlinearity leads to a significant increase in the maximum degree of entanglement of qubits induced by the thermal field, even in the case of high intensities of the resonator field.
考虑原子相干性的克尔介质腔热噪声诱导的两个超导量子比特纠缠
考虑了在克尔非线性存在下,由两个相同的人工原子(量子比特)组成的与理想微波腔量子场模式共振相互作用的系统。对于所考虑的模型,得到了系统双量子位+谐振腔场模式的全密度矩阵的量子Liouville方程的精确解。为了求解演化的量子方程,使用了修饰态的表示,即哈密顿量的特征函数。得到所考虑的模型的一套完整的修饰状态。在它的帮助下,初步找到了量子比特的相干初始态和场的Fock态的演化方程的解,即在谐振腔模式下具有一定数量光子的态。然后,将上述解推广到谐振腔场热态的情况。通过对场变量进行平均,得到了两个量子位元的简化密度矩阵。利用双量子位密度矩阵以解析形式计算量子位纠缠的参数。选择并发性作为量子比特纠缠的定量标准。数值模拟了模型各参数和量子比特初始状态对量子比特一致性的时间依赖性。最有趣的结果似乎是,考虑到克尔非线性模型中量子位的初始相干性,即使在高强度谐振腔场的情况下,热场诱导的量子位的最大纠缠度也会显著增加。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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