Fabry-Perot and Tamm modes hybridization in spatially non-homogeneous magneto-photonic crystal

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We presented the results of studying the features of various resonant modes excitation in a spatially non-homogeneous magnetophotonic crystal with a plasmonic coating. It has been shown that in a such crystal several resonant Fabry-Perot modes and the Tamm plasmon mode are generated at once, which undergo a spectral shift inside the photonic bandgap when the thicknesses of the optical and magnetic layers of magnetophotonic crystal is change.

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作者简介

O. Tomilina

Vernadsky Crimean Federal University

编辑信件的主要联系方式.
Email: olga_tomilina@mail.ru
俄罗斯联邦, Simferopol, 295007

A. Kudryashov

Vernadsky Crimean Federal University

Email: olga_tomilina@mail.ru
俄罗斯联邦, Simferopol, 295007

A. Karavaynikov

Vernadsky Crimean Federal University

Email: olga_tomilina@mail.ru
俄罗斯联邦, Simferopol, 295007

S. Lyashko

Vernadsky Crimean Federal University

Email: olga_tomilina@mail.ru
俄罗斯联邦, Simferopol, 295007

E. Milyukova

Vernadsky Crimean Federal University

Email: olga_tomilina@mail.ru
俄罗斯联邦, Simferopol, 295007

V. Berzhansky

Vernadsky Crimean Federal University

Email: olga_tomilina@mail.ru
俄罗斯联邦, Simferopol, 295007

S. Tomilin

Vernadsky Crimean Federal University

Email: olga_tomilina@mail.ru
俄罗斯联邦, Simferopol, 295007

参考

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2. Fig. 1. Model for calculating the distribution of the thickness of functional layers during magnetron sputtering.

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3. Fig. 2. Results of the experimental study of the distribution of the thickness of the deposited TiO2 layers at different distances l from the target to the substrate: l = 30 (a); 45 (b) and 60 mm (c) (dots – experimental data, solid curve – model analysis).

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4. Fig. 3. Structure of a spatially inhomogeneous MPC with gradient functional layers: general diagram (a), distribution of the thickness of the functional layers along the gradient (b), SEM image of the cross-section of the lower Bragg mirror in the “thin” part (c).

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5. Fig. 4. Transmission spectra of a spatially inhomogeneous 4-pair Bragg mirror GGG/(SiO2/TiO2)4 (a) and a magnetophotonic crystal GGG/(SiO2/TiO2)4/M1/M2/(TiO2/SiO2)4 (b) (the thicknesses of the TiO2/SiO2 layers in the study area are indicated in the legend, the spectra shift is + 0.1).

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6. Fig. 5. Transmission spectra of a spatially inhomogeneous MPC with a plasmonic coating GGG/(SiO2/TiO2)4/M1/M2/(TiO2/SiO2)4/TiO2(buff)/Au (the thicknesses of the TiO2/SiO2 layers in the study area are indicated in the legend, the spectral shift is + 0.02) (a). Spectral position of the Fabry-Perot (FP) resonance modes and Tamm plasmons (TP) in different areas of the spatially inhomogeneous MPC (b).

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7. Fig. 6. Spectra of the magneto-optical Faraday effect in the spatially inhomogeneous GGG/(SiO2/TiO2)4/M1/M2/(TiO2/SiO2)4 MFC in different sections of the gradient (a); comparison of the transmission and magneto-optical rotation spectra in the sections TiO2/SiO2/M1/M2=74/115/67/165 nm (b) and TiO2/SiO2/M1/M2 = 78/122/71/177 nm (c).

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8. Fig. 7. Spectra of the magneto-optical Faraday effect in a spatially inhomogeneous MPC with a plasmonic layer GGG/(SiO2/TiO2)4/M1/M2/(TiO2/SiO2)4/TiO2(buff)/Au in different sections of the gradient (a); comparison of the spectra of magneto-optical rotation in a MPC without a plasmonic layer (Fabry-Perot) and with a plasmonic layer (Fabry-Perot + Tamm) in the sections TiO2/SiO2/M1/M2 = 74/115/67/165 nm (b) and TiO2/SiO2/M1/M2 = 78/122/71/177 nm (c).

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