2021
DOI: 10.1038/s41467-021-26060-x
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Microcavity phonon polaritons from the weak to the ultrastrong phonon–photon coupling regime

Abstract: Strong coupling between molecular vibrations and microcavity modes has been demonstrated to modify physical and chemical properties of the molecular material. Here, we study the less explored coupling between lattice vibrations (phonons) and microcavity modes. Embedding thin layers of hexagonal boron nitride (hBN) into classical microcavities, we demonstrate the evolution from weak to ultrastrong phonon-photon coupling when the hBN thickness is increased from a few nanometers to a fully filled cavity. Remarkab… Show more

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Cited by 34 publications
(35 citation statements)
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“…The maximum splitting that can be reached for a given material turns out to be the well-known value obtained for bulk polaritons, 66 and is independent of cavity geometry. 64 , 65 , 67 , 68 …”
Section: Overview Of Experimental Setupsmentioning
confidence: 99%
“…The maximum splitting that can be reached for a given material turns out to be the well-known value obtained for bulk polaritons, 66 and is independent of cavity geometry. 64 , 65 , 67 , 68 …”
Section: Overview Of Experimental Setupsmentioning
confidence: 99%
“…Since the driving field is weak enough, the hybrid system will stay at the ground state with almost 1 probability, which can be explicitly illustrated by the populations of the lower 9 eigenstates plotted in Fig. 3, where all the parameters are selected within the current experimental conditions [35,63]. Note that the population |C j | 2 at ω d ≈ 1.05ω 0 is about two order of the magnitude less than the population |C 1 | 2 at ω d ≈ 0.74ω 0 in Fig.…”
Section: Parity-conserving Casementioning
confidence: 99%
“…The plasmon then exchanges energy with the phonon mode of the silica slab through electromagnetic coupling. The equation of motion of the system is described by a linear differential equation system 55 58 ( Supporting Information section 6 ). The steady-state solution for the displacement of the driven oscillator gives the polarization induced by the plasmon excitation P = e x and can be written as where Γ j = ω j 2 – iγ j ω – ω 2 is the frequency-dependent response of each oscillator and K = 2 giω is the coupling term.…”
mentioning
confidence: 99%
“…The result of η = 0.13 > 0.1 shows that the hybridization between propagating nanotube Luttinger-liquid plasmons and silica phonons reaches the ultrastrong coupling regime; 59 thus, the damping can be neglected when calculating the eigenfrequencies. While eq 1 is an approximation for the eigenfrequencies, in this case we can formulate the exact solution as 17 , 58 Dispersion curves calculated this way are displayed in Figure 3 b as red dashed lines. They align well with the maxima of the theoretical dispersion map.…”
mentioning
confidence: 99%
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