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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Cavity quantum electrodynamics in superconducting circuits: Susceptibility at elevated temperatures
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Cavity quantum electrodynamics in superconducting circuits: Susceptibility at elevated temperatures

机译:超导电路中的腔量子电动力学:高温下的磁化率

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We study the properties of superconducting electrical circuits, realizing cavity quantum electrodynamics. In particular we explore the limit of strong coupling, low dissipation, and elevated temperatures relevant for current and future experiments. We concentrate on the cavity susceptibility as it can be directly experimentally addressed, i.e., as the impedance or the reflection coefficient of the cavity. To this end we investigate the dissipative Jaynes-Cummings model in the strong coupling regime at high temperatures. The dynamics is investigated within the Bloch-Redfield formalism. At low temperatures, when only the few lowest levels are occupied, the susceptibility can be presented as a sum of contributions from independent level-to-level transitions. This corresponds to the secular (random phase) approximation in the Bloch-Redfield formalism. At temperatures comparable to and higher than the oscillator frequency, many transitions become important and a multiple-peak structure appears. We show that in this regime the secular approximation breaks down, as soon as the peaks start to overlap. In other words, the susceptibility is no longer a sum of contributions from independent transitions. We treat the dynamics of the system numerically by exact diagonalization of the Hamiltonian of the qubit plus up to 200 states of the oscillator. We compare the results obtained with and without the secular approximation and find a qualitative discrepancy already at moderate temperatures.
机译:我们研究了超导电路的特性,实现了腔量子电动力学。特别是,我们探索了与当前和将来的实验相关的强耦合,低耗散和高温的限制。我们专注于腔的磁化率,因为它可以通过实验直接解决,即作为腔的阻抗或反射系数。为此,我们研究了在高温下强耦合状态下的耗散Jaynes-Cummings模型。在Bloch-Redfield形式主义中研究了动力学。在低温下,当仅占据最低的几个最低水平时,磁化率可以表示为独立的水平到水平转换的贡献之和。这对应于Bloch-Redfield形式主义中的世俗(随机阶段)近似。在等于或高于振荡器频率的温度下,许多过渡变得很重要,并且出现了多峰结构。我们表明,在这种情况下,一旦峰开始重叠,则世俗近似分解。换句话说,易感性不再是独立转变的贡献之和。我们通过量子位的哈密顿量的精确对角线化加上振荡器的多达200个状态来数值地对待系统动力学。我们比较在有和没有长期近似的情况下获得的结果,并发现在中等温度下已经存在定性差异。

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