Photonics Research, 2020, 8 (12): 12000A91, Published Online: Nov. 13, 2020
Engineering a light–matter strong coupling regime in perovskite-based plasmonic metasurface: quasi-bound state in the continuum and exceptional points Download: 706次
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Fig. 1. (a) Sketch of the Kretschmann–Raether configuration to investigate guided modes in a stack consisting of encapsulated perovskite thin film of thickness h on a silver substrate. (b), (c), (d) Results of transfer matrix calculations corresponding to the case h = 30 nm : (b), (c) angle-resolved reflectivity spectra in TM-polarized light of (b) passive and (c) active structures; (d) field distribution of the SPP mode shown in (b). (e)–(k) Results of transfer matrix calculations corresponding to the case h = 150 nm : (e)–(h) angle-resolved reflectivity spectra in (e), (g) TM and (f), (h) TE-polarized light of (e), (f) passive and (g), (h) active structures; (i)–(k) field distribution of modes shown in (e) and (f).
Fig. 2. (a) Design of the perovskite metasurface. (b), (d), (e), (f) Folded dispersion of different guided modes extracted from Figs. 1 (b), 1 (e), 1 (f) with period a = 300 nm . (c), (g), (h) Angle-resolved reflectivity spectra obtained from RCWA calculations for (c) h = 30 nm and (g), (h) h = 150 nm . All of these calculations are carried out with a = 300 nm , η = 0.3 , and f = 0.9 .
Fig. 3. (a)–(c) Angle-resolved reflectivity spectra obtained from RCWA calculations for the passive metasurface of (a) f = 0.16 , (b) f = 0.29 , and (c) f = 0.57 . All of these calculations are carried out with a = 300 nm , η = 1 , and h = 30 nm . (d), (e) Field distribution of the dark and bright modes. (f) Ratio of radiative quality factors as a function of k x for different values of the filling fraction f . (g), (h) Spectral position and quality factor of the dark and bright modes at k x = 0 as functions of the filling fraction f .
Fig. 4. (a)–(c) Angle-resolved reflectivity spectra obtained from RCWA calculations for the passive metasurface of (a) f = 0.4 and a = 270 nm , (b) f = 0.51 and a = 267 nm , (c) f = 0.7 and a = 261 nm . All of these calculations are carried out with η = 0.3 and h = 150 nm . (d), (e) Field distribution of the dark and bright modes. (f) Quality factor of the bright and dark modes in (c) as a function of k x . (e), (f) Spectral position and quality factor of the dark and bright modes at k x = k E P = 0.177 μm − 1 as functions of the filling fraction f . In these calculations, the period a is fixed at 265 nm. (i) Dip amplitude of the reflectivity resonance as a function of the spectral detuning to EP.
Fig. 5. (a)–(c) Angle-resolved reflectivity spectra obtained from RCWA calculations for the active metasurface of (a) f = 0.4 and a = 270 nm , (b) f = 0.51 and a = 267 nm , (c) f = 0.7 and a = 261 nm . All of these calculations are carried out with η = 0.3 and h = 150 nm . (d) Quality factor of the dark and bright polaritons in (c) as a function of k x . (g), (h) Spectral position and quality factor of the dark and bright polaritons at k x = k E P = 0.13 μm − 1 as functions of the filling fraction f . In these calculations, the period a is fixed at 265 nm.
Leran Lu, Quynh Le-Van, Lydie Ferrier, Emmanuel Drouard, Christian Seassal, Hai Son Nguyen. Engineering a light–matter strong coupling regime in perovskite-based plasmonic metasurface: quasi-bound state in the continuum and exceptional points[J]. Photonics Research, 2020, 8(12): 12000A91.