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Revised RPS Method for Complex Solution of Multimode Slab Waveguides with Metal layers
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作者 LIJian-jun SHENGuang-di 《Semiconductor Photonics and Technology》 CAS 2004年第3期190-193,共4页
The RPS method,which integrates the real numerical solution, the perturbation solution and the shooting solution reasonably,can obtain the complex solution of a slab waveguide with small gain/loss regions without sear... The RPS method,which integrates the real numerical solution, the perturbation solution and the shooting solution reasonably,can obtain the complex solution of a slab waveguide with small gain/loss regions without searching the root in the entire complex plan.A revision to the RPS method is presented so that it can deal with the waveguide including large gain/loss regions.The application indicated that the simulation results are precise. 展开更多
关键词 Optical waveguides slab waveguides Simulation RPS method
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Generation of lossy mode resonances(LMR)using perovskite nanofilms
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作者 Dayron Armas Ignacio R.Matias +4 位作者 M.Carmen Lopez-Gonzalez Carlos Ruiz Zamarreño Pablo Zubiate Ignacio del Villar Beatriz Romero 《Opto-Electronic Advances》 SCIE EI CAS CSCD 2024年第2期33-40,共8页
The results presented here show for the first time the experimental demonstration of the fabrication of lossy mode resonance(LMR) devices based on perovskite coatings deposited on planar waveguides. Perovskite thin fi... The results presented here show for the first time the experimental demonstration of the fabrication of lossy mode resonance(LMR) devices based on perovskite coatings deposited on planar waveguides. Perovskite thin films have been obtained by means of the spin coating technique and their presence was confirmed by ellipsometry, scanning electron microscopy, and X-ray diffraction testing. The LMRs can be generated in a wide wavelength range and the experimental results agree with the theoretical simulations. Overall, this study highlights the potential of perovskite thin films for the development of novel LMR-based devices that can be used for environmental monitoring, industrial sensing, and gas detection, among other applications. 展开更多
关键词 PEROVSKITE thin films slab waveguide lossy mode resonance
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Propagation of Electromagnetic Waves in Slab Waveguide Structure Consisting of Chiral Nihility Claddings and Negative-Index Material Core Layer
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作者 Alaa N. Abu HELAL Sofyan A. TAYA Khitam Y. ELWASIFE 《Photonic Sensors》 SCIE EI CAS CSCD 2018年第2期176-187,共12页
The dispersion equation of an asymmetric three-layer slab waveguide, in which all layers are chiral materials is presented. Then, the dispersion equation of a symmetric slab waveguide, in which the claddings are chira... The dispersion equation of an asymmetric three-layer slab waveguide, in which all layers are chiral materials is presented. Then, the dispersion equation of a symmetric slab waveguide, in which the claddings are chiral materials and the core layer is negative index material, is derived. Normalized cut-off frequencies, field profile, and energies flow of right-handed and left-handed circularly polarized modes are derived and plotted. We consider both odd and even guided modes. Numerical results of guided low-order modes are provided. Some novel features, such as abnormal dispersion curves, are found. 展开更多
关键词 slab waveguides chiral materials left-handed materials
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Reactive ion etching of Ti-diffused LiNbO_3 slab waveguides
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作者 吴建杰 李金洋 +1 位作者 要彦清 祁志美 《Journal of Semiconductors》 EI CAS CSCD 2013年第8期188-192,共5页
Reactive ion etching(RIE) of LiNbO_3(LN) in SF_6 plasma atmosphere was studied for optimizing the preparation conditions for LN ridge waveguides.The samples to be etched are Ti-diffused LN slab waveguides overlaid... Reactive ion etching(RIE) of LiNbO_3(LN) in SF_6 plasma atmosphere was studied for optimizing the preparation conditions for LN ridge waveguides.The samples to be etched are Ti-diffused LN slab waveguides overlaid with a chromium film mask that has a Mach-Zehnder interferometer(MZI) array pattern.The experimental results indicate that the LN-etching rate(R_(LN)) and the Cr-etching rate(R_(Cr)) as well as the rate ratio R_(LN)/R_(Cr) increase with either increasing the radio-frequency(RF) power at a given SF_6 flow rate or increasing the SF_6 flow rate at a fixed RF power.The maximum values of R_(LN) = 43.2 nm/min and R_(LN)/R_(Cr) = 3.27 were achieved with 300 W RF power and 40 sccm SF_6 flow.When the SF_6 flow rate exceeds 40 sccm,an increase in the flow rate causes the etching rates and the rate ratio to decrease.The scanning electron microscope images of the LN ridge prepared after~20 min etching show that the ridge height is 680 nm and the sidewall slope angle is about 60°. 展开更多
关键词 reactive ion etching Ti-diffused LiNbO_3 slab waveguide optimal etching parameters ridge waveguide
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