论文标题
微波QED中的结合状态:从波导到空腔状态的交叉状态
Bound states in microwave QED: Crossover from waveguide to cavity regime
论文作者
论文摘要
单量子级别的轻度相互作用是许多对现代量子技术基本重要性的核心。量子与电磁场模式的单个光子的强相互作用由腔/电路电动力学(QED)制度描述,这是量子计算最先进的平台之一。波导QED的相反机制与无限一维空间中的连续模式相互作用也是最近的研究的重点,揭示了新型量子现象。尽管证明了波导QED的几个关键特征,但从实验可实现的有限大小系统到理论上假定的无限设备尺寸的过渡既不是有道理的,也不是完全理解的。在本文中,我们制定了一个统一的理论,该理论在一组最小的标准近似值中解释了所有参数域中系统的物理边界。考虑到自然表现出低频截止的矩形波导中的两个Qubit,我们能够考虑无限数量的模式,并获得对波导透射的准确描述,波导透射率,Qubit-Photon结合状态的寿命以及两个Qubit-Photon边界之间的交换相互作用。为了进行验证,我们将我们的理论与矩形波导中两个超导Qub的实验数据进行了比较,以证明波导QED的无限尺寸极限如何在有限大小的系统中出现。我们的理论可以直接扩展到其他波导,例如光子晶体和耦合腔阵列。
Light-matter interaction at the single-quantum level is the heart of many regimes of high fundamental importance to modern quantum technologies. Strong interaction of a qubit with a single photon of an electromagnetic field mode is described by the cavity/circuit electrodynamics (QED) regime which is one of the most advanced platforms for quantum computing. The opposite regime of the waveguide QED, where qubits interact with a continuum of modes in an infinite one-dimensional space, is also at the focus of recent research revealing novel quantum phenomena. Despite the demonstration of several key features of waveguide QED, the transition from an experimentally realizable finite-size system to the theoretically assumed infinite device size is neither rigorously justified nor fully understood. In this paper, we formulate a unifying theory which under a minimal set of standard approximations accounts for physical boundaries of a system in all parameter domains. Considering two qubits in a rectangular waveguide which naturally exhibits a low frequency cutoff we are able to account for infinite number of modes and obtain an accurate description of the waveguide transmission, a life-time of a qubit-photon bound state and the exchange interaction between two qubit-photon bounds states. For verification, we compare our theory to experimental data obtained for two superconducting qubits in a rectangular waveguide demonstrating how the infinite size limit of waveguide QED emerges in a finite-size system. Our theory can be straightforwardly extended to other waveguides such as the photonic crystal and coupled cavity arrays.