Surface state peculiarities in one-dimensional photonic crystal interfaces

Виноградов, А. П.; Dorofeenko, A. V.; Erokhin, Sergey; Inoue, M.; Lisyansky, A. A.; Merzlikin, A. M.; Granovsky, A.B.

doi:10.1103/physrevb.74.045128

Cited by 214 publications

(125 citation statements)

References 27 publications

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“…8 shows the transmittivity versus frequency at different number of periods at the left and right of the defect layer (the whole number of periods is constant). It can be seen that due to a resonance tunneling of an electromagnetic wave through the defectless part of the structure, a narrow transmittivity peak appears [5,6]. The presence of defect layers in the periodic structure causes the appearance of defect modes in the forbidden bands.…”

Section: Transmission Spectra Of the Structure With Periodicity Breakmentioning

confidence: 99%

“…These structures can easily change their characteristics in an external magnetic field. The results of theoretical investigations of spaceinhomogeneous magnetic media were presented in [1][2][3][4][5][6][7][8][9]. It was considered the reflection from the semiinfinite periodically layered structure composed of alternating semiconductor and insulator layers [10].…”

Section: Introductionmentioning

confidence: 99%

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Transmission Spectra in Ferrite-Semiconductor Periodic Structure

Shramkova¹

2009

PIER M

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Abstract-The specific features of TE-wave propagation in a structure fabricated by periodic alternating ferrite and semiconductor layers are investigated.Dispersion characteristics of eigenwaves are calculated. The transmission spectra of an electromagnetic wave oblique incident from the uniform medium onto the multilayer periodic ferrite-semiconductor structure is considered. The features of transmission spectra of the structure with periodicity breakdown are studied.

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Section: Transmission Spectra Of the Structure With Periodicity Breakmentioning

confidence: 99%

Section: Introductionmentioning

confidence: 99%

Transmission Spectra in Ferrite-Semiconductor Periodic Structure

Shramkova¹

2009

PIER M

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“…eig,Bz eig (1) where k x eig,Bz is the x-component of the eigenmode's wavevector in the first Brillouin zone, k x eig is the x-component of the eigenmode's wavevector in the absence of the array of slits, π = G T 2 / is the reciprocal lattice constant, and n is an integer number ('diffraction order'). In order to couple the Tamm state and the waveguide mode of interest at the specified wavelength, the following condition must hold true (n might be different for the Tamm state and the waveguide mode):…”

Section: Eigenmodes Of the Dielectric Photonic Crystal Covered With Amentioning

confidence: 99%

“…">IntroductionThe optical Tamm state, which can occur either on the boundary of two photonic crystals [1,2] or on the boundary of a photonic crystal and a metal film [3][4][5][6][7][8][9][10][11][12], has recently attracted attention of researchers in nano-optics community. The optical Tamm state in a system with a photonic crystal covered with a metal film is especially interesting because it allows one to combine its complicated physics with the rich physics of plasmon surface waves.…”

mentioning

confidence: 99%

Fano resonances in a photonic crystal covered with a perforated gold film and its application to bio-sensing

Klimov

Pavlov

Treshin

et al. 2017

J. Phys. D: Appl. Phys.

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IntroductionThe optical Tamm state, which can occur either on the boundary of two photonic crystals [1,2] or on the boundary of a photonic crystal and a metal film [3][4][5][6][7][8][9][10][11][12], has recently attracted attention of researchers in nano-optics community. The optical Tamm state in a system with a photonic crystal covered with a metal film is especially interesting because it allows one to combine its complicated physics with the rich physics of plasmon surface waves. Since the first experimental demonstration [3], the optical Tamm state is an object of numerous researches. In particular, interaction of the Tamm state and a surface plasmon wave has been already shown [4,5]. Besides, the scheme of a sensor which is sensitive to the change of a refractive index based on the optical Tamm state has been offered [6,7]. Recently, in a system consisting of a photonic crystal and a perforated metal film, effects of the extraordinary transmission of light and huge asymmetry of transmission related to the optical Tamm state have been discovered [8,9]. The optical Tamm state has been investigated in the presence of nonlinear effects, particularly as a lasing mode of the nanolaser [10], it has been used to enhance the second harmonic generation [11] and to control spontaneous radiation of quantum emitters [12].In this work, we investigate another effect associated with the optical Tamm state. The photonic crystal necessary to observe an optical Tamm resonance supports the propagation of a set of waveguide modes. In this paper, we show that it is possible to achieve an interaction between the waveguide modes of the photonic crystal and the Tamm state with the help of a periodic lattice of slits in a metal film. We show that this interaction results in the Fano resonance, which is a typical sign of the interaction of high-quality dark and lowquality bright modes. In spite of the fact that the research of Fano resonance in photonic and plasmonic structures is a hot topic now [13-18], we do not know any investigation devoted AbstractOptical properties of the photonic crystal covered with a perforated metal film were investigated and the existence of the Fano-type resonances was shown. The Fano resonances originate from the interaction between the optical Tamm state and the waveguide modes of the photonic crystal. It manifests itself as a narrow dip in a broad peak in the transmission spectrum related to the optical Tamm state. The design of a sensor based on this Fano resonance that is sensitive to the change of the environment refractive index is suggested.

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“…We may also point out that there are significant differences with respect to localization when compared to Tamm states, characterized at the surface of dielectric multilayers. 16,17 The article is organized as follows. After this introduction, Sec.…”

Section: Introductionmentioning

confidence: 99%

Low-Qwhispering gallery modes in anisotropic metamaterial shells

et al. 2013

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Anisotropic and inhomogeneous metamaterial shells are studied in order to exploit all their resonant mode richness. These multilayer structures are based on a cylindrical distribution of radially dependent constitutive parameters including an inner void cavity. Shell, cavity, and whispering gallery modes are characterized, and special attention is paid to the latter ones. The whispering gallery modes are created at the boundary layers of the shell with the background. Energy localization is produced with highly radiative characteristics when the localization takes place at the external layer. These low-Q resonant states have frequencies that are independent of the shell thickness. However, their quality factors can be controlled by the number of layers forming the shell, which allows confining electromagnetic waves at the interface layers (internal or external), and make them suitable for the harvesting of electromagnetic energy.

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Surface state peculiarities in one-dimensional photonic crystal interfaces

Cited by 214 publications

References 27 publications

Transmission Spectra in Ferrite-Semiconductor Periodic Structure

Transmission Spectra in Ferrite-Semiconductor Periodic Structure

Fano resonances in a photonic crystal covered with a perforated gold film and its application to bio-sensing

Low-Qwhispering gallery modes in anisotropic metamaterial shells

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