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Non-Hermitian Hamiltonian approach to the microwave transmission through a one-dimensional qubit chain

机译:非埃尔米特哈密顿方法通过一维量子位链进行微波传输

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摘要

We investigate the propagation of microwave photons in a one-dimensional open waveguide interacting with a number of artificial atoms (qubits). Within the formalism of projection operators and a non-Hermitian Hamiltonian approach we develop a one-photon approximation scheme for the calculation of the transmission and reflection factors of the microwave signal in a waveguide which contains an arbitrary number N of noninteracting qubits. We considered in detail the resonances and photon-mediated entanglement for two and three qubits in a chain. We showed that in the non-Markovian case the resonance widths, which define the decay rates of the entangled state, can be much smaller than the decay width of an individual qubit. It is also shown that for identical qubits in the long-wavelength limit a coherent superradiant state is formed with the width being equal to the sum of the widths of spontaneous transitions of N individual qubits. The results obtained in the paper are of general nature and can be applied to any type of qubits. The specific properties of the qubit are only encoded in the two parameters: the qubit energy Omega and the rate of spontaneous emission Gamma.
机译:我们研究了一维开放波导中与许多人造原子(量子位)相互作用的微波光子的传播。在投影算子和非Hermitian哈密顿方法的形式主义中,我们开发了一种单光子近似方案,用于计算包含任意数量的N个非相互作用量子位的波导中微波信号的传输和反射因子。我们详细考虑了链中两个和三个量子位的共振和光子介导的纠缠。我们表明,在非马尔可夫情形下,确定纠缠态衰减率的共振宽度可能比单个量子位的衰减宽度小得多。还显示出,对于长波长限制中的相同量子位,形成了相干的超辐射态,其宽度等于N个单个量子位的自发跃迁的宽度之和。本文获得的结果具有一般性,可以应用于任何类型的量子位。量子位的特定属性仅在两个参数中编码:量子位能量Omega和自发发射Gamma率。

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