2021
DOI: 10.1103/physrevb.104.125446
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Strong coupling between excitons in a two-dimensional atomic crystal and quasibound states in the continuum in a two-dimensional all-dielectric asymmetric metasurface

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Cited by 42 publications
(18 citation statements)
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“…The Q-BIC mode generated by the asymmetric structure means that destroy the metasurface consisting of C 4V symmetric atomic arrays. This symmetry breaking leads to the leakage of previously protected bound states, resulting in the formation of Q-BIC accompanied by radiation losses [18][19][20][21][22]. Yang et al leveraged the asymmetric field distribution in the Q-BIC by purposefully truncating the tips of the constituent elliptical nano-silicon bars to improve the resonance performance of the symmetry-breaking Q-BIC system and enhance the trapping of subwavelength particles [23].…”
Section: Introductionmentioning
confidence: 99%
“…The Q-BIC mode generated by the asymmetric structure means that destroy the metasurface consisting of C 4V symmetric atomic arrays. This symmetry breaking leads to the leakage of previously protected bound states, resulting in the formation of Q-BIC accompanied by radiation losses [18][19][20][21][22]. Yang et al leveraged the asymmetric field distribution in the Q-BIC by purposefully truncating the tips of the constituent elliptical nano-silicon bars to improve the resonance performance of the symmetry-breaking Q-BIC system and enhance the trapping of subwavelength particles [23].…”
Section: Introductionmentioning
confidence: 99%
“…While most of the milestones of polaritonic physics have been achieved with excitonic materials operating at cryogenic temperatures (≈10 K), recent progress in materials science has promoted many polaritonic demonstrations at room temperature with a wide variety of high bandgap semiconductors, ranging from GaN, [24,25] ZnO, [26] to organic semiconductors, [27,28] and transition metal dichalcogenide monolayers, [29,30] as well as perovskite materials. [31][32][33][34][35][36][37][38][39][40][41] Very recently, the strong coupling regime between photonic BICs and excitonic resonances has been theoretically suggested, [42][43][44][45] with two experimental demonstrations. [46,47] The result of such a coupling is the formation of polariton-BICs (pol-BICs): hybrid excitations that are completely decoupled from the radiative continuum.…”
Section: Introductionmentioning
confidence: 99%
“…43 Liang et al designed a periodical silicon-bar-pair array to realize a Rabi splitting of 34 meV. 44 However, the schemes mentioned above are merely used for realizing strong coupling between photonic resonance and exciton in monolayer TMDCs. Owing to the ultrathin nature of a TMDC monolayer, the interactions between TMDC monolayer and light are typically extremely weak.…”
Section: Introductionmentioning
confidence: 99%