Bound states in the continuum and Fano resonances in the strong mode coupling regime
暂无分享,去创建一个
K. L. Koshelev | Z. F. Sadrieva | K. B. Samusev | A. A. Bogdanov | S. A. Gladyshev | M. F. Limonov | M. V. Rybin | P. V. Kapitanova | Yu.S. Kivshar | Y. Kivshar | A. Bogdanov | Z. Sadrieva | P. Kapitanova | K. Samusev | M. Limonov | M. Rybin | K. Koshelev | S. Gladyshev
[1] Larry D. Travis,et al. T-matrix computations of light scattering by large spheroidal particles , 1994 .
[2] P. T. Leung,et al. Quasinormal-mode expansion for waves in open systems , 1998 .
[3] P. Barber. Absorption and scattering of light by small particles , 1984 .
[4] Steven G. Johnson,et al. Multipole-cancellation mechanism for high-Q cavities in the absence of a complete photonic band gap , 2001 .
[5] C. Sauvan,et al. Fano resonances in photonic crystal slabs near optical bound states in the continuum , 2016 .
[6] C. C. Lam,et al. Effect of perturbations on the widths of narrow morphology-dependent resonances in Mie scattering , 1991 .
[7] Elena Semouchkina,et al. Mie scattering as a cascade of Fano resonances. , 2013, Optics express.
[8] J. Neumann,et al. Uber merkwürdige diskrete Eigenwerte. Uber das Verhalten von Eigenwerten bei adiabatischen Prozessen , 1929 .
[9] Shanhui Fan,et al. Temporal coupled-mode theory and the presence of non-orthogonal modes in lossless multimode cavities , 2004, IEEE Journal of Quantum Electronics.
[10] Arkady M. Satanin,et al. RESONANT TUNNELING IN A QUANTUM WAVEGUIDE : EFFECT OF A FINITE-SIZE ATTRACTIVE IMPURITY , 1999 .
[11] Andrea Alù,et al. Embedded photonic eigenvalues in 3D nanostructures , 2014 .
[12] A. Matsko,et al. Optical resonators with whispering-gallery modes-part I: basics , 2006, IEEE Journal of Selected Topics in Quantum Electronics.
[13] Yuri S. Kivshar,et al. Fano resonances in photonics , 2017, Nature Photonics.
[14] K. Vahala. Optical microcavities , 2003, Nature.
[15] J. Wiersig. Formation of long-lived, scarlike modes near avoided resonance crossings in optical microcavities. , 2006, Physical review letters.
[16] Anatolii N Oraevsky,et al. Whispering-gallery waves , 2002 .
[17] B. Chichkov,et al. Optical theorem and multipole scattering of light by arbitrarily shaped nanoparticles , 2016 .
[18] E. Bulgakov,et al. Propagating Bloch bound states with orbital angular momentum above the light line in the array of dielectric spheres. , 2017, Journal of the Optical Society of America. A, Optics, image science, and vision.
[19] J. Ganne,et al. Resonance continuum coupling in high-permittivity dielectric metamaterials , 2010 .
[20] E. Tutuc,et al. Photonic-crystal exciton-polaritons in monolayer semiconductors , 2017, Nature Communications.
[21] A. Matsko,et al. Optical resonators with whispering-gallery modes-part II: applications , 2006, IEEE Journal of Selected Topics in Quantum Electronics.
[22] Keqian Zhang,et al. Electromagnetic Theory for Microwaves and Optoelectronics , 2007 .
[23] L. Brillouin. Les problèmes de perturbations et les champs self-consistents , 1932 .
[24] V. Weisskopf,et al. Effects of Configuration Interaction on Intensities and Phase Shifts , 2001 .
[25] F. Lederer,et al. Multipole analysis of meta-atoms , 2011 .
[26] Transition from Optical Bound States in the Continuum to Leaky Resonances: Role of Substrate and Roughness , 2017 .
[27] R. More. THEORY OF DECAYING STATES. , 1971 .
[28] M. Segev,et al. Experimental observation of optical bound states in the continuum. , 2011, Physical review letters.
[29] K. Vahala,et al. High-Q surface-plasmon-polariton whispering-gallery microcavity , 2009, Nature.
[30] Yuri Kivshar,et al. Optical physics: Supercavity lasing , 2017, Nature.
[31] Friedrich,et al. Interfering resonances and bound states in the continuum. , 1985, Physical review. A, General physics.
[32] Gael Favraud,et al. Fundamental and high-order anapoles in all-dielectric metamaterials via Fano–Feshbach modes competition , 2017, Nanotechnology.
[33] A. Kildishev,et al. Formation of Bound States in the Continuum in Hybrid Plasmonic-Photonic Systems. , 2018, Physical review letters.
[34] T. Lepetit,et al. Controlling multipolar radiation with symmetries for electromagnetic bound states in the continuum , 2014 .
[35] A. Crespi,et al. Observation of surface states with algebraic localization. , 2013, Physical review letters.
[36] Young,et al. Time-independent perturbation for leaking electromagnetic modes in open systems with application to resonances in microdroplets. , 1990, Physical review. A, Atomic, molecular, and optical physics.
[37] Extinction cross section measurements , 2008 .
[38] Philippe Regreny,et al. Subwavelength plasmonic lasing from a semiconductor nanodisk with silver nanopan cavity. , 2010, Nano letters.
[39] Sergei V. Shabanov,et al. Electromagnetic bound states in the radiation continuum for periodic double arrays of subwavelength dielectric cylinders , 2010, 1005.2962.
[40] L. Fonda. Bound states embedded in the continuum and the formal theory of scattering , 1963 .
[41] T. Asano,et al. High-Q photonic nanocavity in a two-dimensional photonic crystal , 2003, Nature.
[42] G. Xiao,et al. Fano resonances in core-shell particles with high permittivity covers , 2016, 2016 Progress in Electromagnetic Research Symposium (PIERS).
[43] M. Soljačić,et al. Topological nature of optical bound states in the continuum. , 2014, Physical Review Letters.
[44] E. Bulgakov,et al. Bound states in the continuum in photonic waveguides inspired by defects , 2008 .
[45] U. Kaatze. Complex Permittivity of Water as a Function of Frequency and Temperature , 1989 .
[46] A. Borisov,et al. Bound States in the continuum in photonics. , 2008, Physical review letters.
[47] A. S. Pilipchuk,et al. Bound states in the continuum in open acoustic resonators , 2015, Journal of Fluid Mechanics.
[48] Wideband Measurements of the Forward RCS and the Extinction Cross Section , 2012 .
[49] M. Mishchenko,et al. Light scattering by size-shape distributions of randomly oriented axially symmetric particles of a size comparable to a wavelength. , 1993, Applied optics.
[50] N. Engheta,et al. Near-zero refractive index photonics , 2017, Nature Photonics.
[51] E. Muljarov,et al. Brillouin-Wigner perturbation theory in open electromagnetic systems , 2010, 1205.4924.
[52] Y. Kivshar,et al. Surface bound states in the continuum. , 2011, Physical review letters.
[53] R. Parker,et al. Resonance effects in wake shedding from parallel plates: Some experimental observations , 1966 .
[54] Benjamin Gallinet,et al. Ab initio theory of Fano resonances in plasmonic nanostructures and metamaterials , 2011, 1105.2503.
[55] S. Matinyan,et al. To the theory of unstable states , 2008, 0809.2520.
[56] A. Miroshnichenko,et al. Giant in-particle field concentration and Fano resonances at light scattering by high-refractive-index particles , 2015, 1511.02931.
[57] B. Luk’yanchuk,et al. Optically resonant dielectric nanostructures , 2016, Science.
[58] B. Chichkov,et al. All-dielectric nanophotonics: the quest for better materials and fabrication techniques , 2017, 1702.00677.
[59] J. Wiersig,et al. Goos-Hänchen shift and localization of optical modes in deformed microcavities. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.
[60] Andrey Bogdanov,et al. High-Q Supercavity Modes in Subwavelength Dielectric Resonators. , 2017, Physical review letters.
[61] Steven G. Johnson,et al. Observation of trapped light within the radiation continuum , 2013, Nature.
[62] Y. Kivshar,et al. Switching from Visibility to Invisibility via Fano Resonances: Theory and Experiment , 2014, Scientific Reports.
[63] R. Parker. Resonance effects in wake shedding from parallel plates: Calculation of resonant frequencies , 1967 .