Anton S. Belashov, Evgeny S. Andrianov, Alexander A. Zyablovsky
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引用次数: 0
摘要
空穴-单原子 "系统中的强耦合和超强耦合对基础物理学和应用物理学都具有重大意义。人们认为,空穴模式与原子之间耦合强度的增加首先会导致从弱耦合到强耦合的过渡,其次会导致超强耦合。在本文中,我们驳斥了这一普遍观点,并证明了不同阶相关函数的耦合机制之间的转变发生在不同的序列中。我们证明,对于 n 阶相关函数,过渡到强耦合机制需要的耦合强度大约是一阶相关函数的 n2/3 倍。与此相反,向超强耦合机制过渡时,n-阶相关函数的动力学耦合强度要小于一阶相关函数的动力学耦合强度。因此,测量高阶相关函数更容易观察到 "空穴模式-单原子 "中的超强耦合。
Manifestation of strong and ultra-strong coupling in high-order correlation functions
Strong and ultra-strong coupling in a “cavity–single atom” system is of great interest for both fundamental and applied physics. It is considered that the increase in the coupling strength between a cavity mode and an atom leads, first, to transition from weak to strong coupling and, second, to the ultra-strong coupling regime. In this paper, we refute this common opinion and demonstrate that the transitions between the coupling regimes occur in different sequences for the correlation functions of different orders. We show that for n-th order correlation functions, the transition to the strong coupling regime requires a coupling strength approximately n2/3 times greater than the one for first order correlation functions. In contrast, the transition to the ultra-strong coupling regime manifests in the dynamics of n-th order correlation functions at less coupling strength than in the dynamics of first order correlation functions. As a result, the measurement of high-order correlation functions makes it easier to observe the ultra-strong coupling in “cavity mode–single atom.”