Description of ultrastrong light-matter interaction through coupled harmonic oscillator models and their connection with cavity-QED Hamiltonians

被引:0
|
作者
Muniain, Unai [1 ]
Aizpurua, Javier [1 ,3 ,4 ]
Hillenbrand, Rainer [3 ,4 ,5 ]
Martin-Moreno, Luis [6 ,7 ]
Esteban, Ruben [1 ,2 ]
机构
[1] Donostia Int Phys Ctr, Paseo Manuel Lardizabal 4, Donostia San Sebastian 20018, Spain
[2] CSIC UPV EHU, Ctr Fis Mat CFM MPC, Paseo Manuel Lardizabal 5, Donostia San Sebastian 20018, Spain
[3] Basque Fdn Sci, IKERBASQUE, Maria Diaz Haro 3, Bilbao 48013, Spain
[4] Univ Basque Country UPV EHU, Dept Elect & Elect, Leioa 48940, Spain
[5] C nanoGUNE BRTA, Tolosa Hiribidea 76, Donostia San Sebastian 20018, Spain
[6] Univ Zaragoza, CSIC, Inst Nanociencia & Mat Aragon INMA, Zaragoza 50009, Spain
[7] Univ Zaragoza, Dept Fis Mat Condensada, Zaragoza 50009, Spain
关键词
quantum nanophotonics; ultrastrong coupling; transverse and longitudinal fields; Coulomb coupling; Reststrahlen band; nanocavities; SPONTANEOUS EMISSION; INDUCED TRANSPARENCY; 2-LEVEL ATOMS; REGIME; PHOTON; REALIZATION; POLARITONS; CHEMISTRY; CROSSINGS; PLASMONS;
D O I
10.1515/nanoph-2024-0528
中图分类号
TB3 [工程材料学];
学科分类号
0805 ; 080502 ;
摘要
Classical coupled harmonic oscillator models are capable of describing the optical and infrared response of nanophotonic systems where a cavity photon couples to dipolar matter excitations. The distinct forms of coupling adopted in these classical models lead to different results in the ultrastrong coupling regime. To clarify the specific classical model required to address particular configurations, we establish a connection between each oscillator model and the equivalent cavity Quantum Electrodynamics description. We show that the proper choice of coupled harmonic oscillator model depends on the presence or absence of the diamagnetic term in the quantum models, linked to whether transverse or longitudinal electromagnetic fields mediate the coupling. This analysis also shows how to exploit the classical oscillator models to extract measurable information of the optical response, as demonstrated in three canonical photonic systems, and to describe the opening of the Reststrahlen band in the bulk dispersion of phononic materials.
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页数:22
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