2020
DOI: 10.1016/bs.semsem.2020.10.002
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Ultrastrong light–matter coupling in semiconductors

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Cited by 12 publications
(9 citation statements)
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“…The USC regime arises when g becomes a significant fraction of the bare uncoupled matter and light frequency at zero detuning, ω 0 , conventionally defined as g 0.1ω 0 . Nontrivial vacuum electromagnetic fluctuations can interact with the matter and modify the properties of the system in the USC regime [121]. In this subsection, we review the enhancement of single-photon emission in CNT systems in the WC regime using different cavity designs.…”
Section: Cavity Enhancement Of Single-photon Emissionmentioning
confidence: 99%
“…The USC regime arises when g becomes a significant fraction of the bare uncoupled matter and light frequency at zero detuning, ω 0 , conventionally defined as g 0.1ω 0 . Nontrivial vacuum electromagnetic fluctuations can interact with the matter and modify the properties of the system in the USC regime [121]. In this subsection, we review the enhancement of single-photon emission in CNT systems in the WC regime using different cavity designs.…”
Section: Cavity Enhancement Of Single-photon Emissionmentioning
confidence: 99%
“…Interestingly, these two modes exhibit anticrossing behaviors, which is an indication of strong coupling/hybridization. [81][82][83] To explain the hybridization between the qFM and qAFM modes, the authors developed a microscopic model, which includes interactions between spins in the two sublattices, their symmetric exchange and antisymmetric exchange, the singleion anisotropies, and the Zeeman interaction. The system was effectively described by two coupling strengths g 1 (corotating coupling strength) and g 2 (counter-rotating coupling strength).…”
Section: Magnons 331 Ultrastrong Magnon-magnon Coupling In Yfeomentioning
confidence: 99%
“…As it describes the collective degrees of freedom of a set of two-level systems (qubits), the Dicke Hamiltonian offers a general description of the spin–boson interaction. Additionally, it constitutes a paradigmatic example for the study of the ultra-strong coupling (USC) regime [ 13 , 14 , 15 ] Consequently, the model has found a great reception in the description of several setups, mainly in the context of quantum information [ 16 , 17 , 18 , 19 ]. In recent years, it has been experimentally realized in a broad range of tunable systems, from Bose–Einstein condensates in optical lattices [ 7 , 20 , 21 , 22 , 23 ], superconducting qubits [ 24 , 25 , 26 ] to cavity-assisted Raman transitions [ 27 , 28 ].…”
Section: Introductionmentioning
confidence: 99%