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Number of results: 23
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Abstract

Optical waveguides (WGs) are widely used as interconnects in integrated optical circuits both for telecommunication and sensing applications. There are different kind of optical WG designs that offers different guiding parameters, opening a vast number of possibilities. A silica-titania (SiO2:TiO2) rib WG is discussed and examined by a numerical analysis in this article with a great emphasis on the analysis of bending losses and optimization. A modal analysis for different basic parameters of the WG is presented with a detailed wavelength-based modal analysis. Various potential fabrication methods are discussed, however, a sol-gel method and dip-coating deposition technique are proposed for the low-cost development of such WGs. Moreover, an approach towards minimizing the bending losses by adding an upper cladding layer on the rib WG is presented and described.
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Authors and Affiliations

Muhammad Shahbaz
1
ORCID: ORCID
Łukasz Kozlowski
1
Muhammad A. Butt
1
ORCID: ORCID
Ryszard Piramidowicz
1
ORCID: ORCID

  1. Institute of Microelectronics and Optoelectronics, Warsaw University of Technology, Koszykowa 75, 00-662 Warszawa, Poland
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Abstract

Flow fields could be of great interest in the study of sound propagation in aeroengines. For ducts with rigid boundaries, the fluid-resonant category may contribute significantly to unwanted noise. An understanding of the multi-modal propagation of acoustic waves in ducts is of practical interest for use in the control of noise in, for example, aero-engines, automotive exhaust and heating or ventilation systems. The purpose of our experiments was to test the acoustic energy transmission of duct modes based on studies carried out by the sound intensity technique. Sound intensity patterns in circular duct are discussed of modal energy analysis with particular reference to proper orthogonal decomposition and dynamic mode decomposition. The authors try to justify some advantages of the sound intensity experimental research in this area. In the paper, the wide-band sound signal propagated from source approximated with loudspeaker in hard-walled duct is imaged using a sound intensity - based approach. For a simple duct geometry, the sound intensity field is examined visually and by performing a modal decomposition greater insight into the acoustic structures is obtained. The image of sound intensity fields below and above “cut-off” frequency region are found to compare acoustic modes which might resonate in duct.

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Authors and Affiliations

Stefan Weyna
Witold Mickiewicz
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Abstract

In this study a metal clad waveguide sensor with a metamaterial guiding layer is analyzed. Sensitivity of the proposed sensor is derived using dispersion and Fresenal’s equations for waveguiding mode and reflection mode. While efficiently analyzing and comparing the results with the existing one, some interesting findings are achieved. It is observed that the proposed sensor shows larger cover layer sensitivity and larger adlayer sensitivity compared to the dielectric guiding layer sensor due to adsorbtive properties of metamaterial. Henceforth, it concludes that the proposed sensor shows sensitivity improvement over a dielectric guiding layer sensor.

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Authors and Affiliations

A. Upadhyay
Y.K. Prajapati
R. Tripathi
V. Singh
J.P. Saini
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Abstract

The normal modes cannot be extracted even in the Pekeris waveguide when the source-receiver distance is very close. This paper introduces a normal mode extraction method based on a dedispersion transform (DDT) to solve this problem. The method presented here takes advantage of DDT, which is based on the waveguide invariant such that the dispersion associated with all of the normal modes is removed at the same time. After performing DDT on a signal received in the Pekeris waveguide, the waveform of resulting normal modes is very close to the source signal, each with different position and amplitude. Each normal mode can be extracted by determining its position and amplitude parameters by applying particle swarm optimization (PSO). The waveform of the extracted normal mode is simply the waveform of the source signal; the real waveform of the received normal mode can then be recovered by applying dispersion compensation to the source signal. The method presented needs only one receiver and is verified with experimental data
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Authors and Affiliations

Guang-Bing Yang
Lian-Gang Lü
Da-Zhi Gao
Ying Jiang
Hong-Ning Liu
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Abstract

The possibility of acoustic wave propagation in optical waveguides creates new prospects for simultaneous transmission of laser beams and ultrasonic waves. Combined laser-ultrasonic technology could be useful in e.g. surgical treatment. The article presents the results of experimental studies of transmission of ultrasonic wave in optical fibres, the core of which is doped by 7.5% of TiO2, using a sandwich-type transducer. It also presents amplitude characteristics of an ultrasonic signal propagated in the optical fibre. Authors studied the effect which the length of the fibre has on the achieved output signal amplitudes. They presented the relation of the output signal amplitude from a capacitive sensor to the power applied to the sandwich-type transducer. The obtained results were compared with the results produced when using an optical fibre with a core doped by 3% of GeO2, in order to select optical fibre suitable for simultaneous transmission of ultrasonic waves and laser rays.

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Authors and Affiliations

Sylwia Muc
Tadeusz Gudra
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Abstract

In this paper the overview of the recent study on the rare-earth activated waveguides performed in the Optoelectronic Department of IMiO is presented. We reported on the development of rare earth-doped fluorozirconate (ZBLAN) glass fibers that allow a construction of a new family of visible and ultraviolet fiber lasers pumped by upconversion. Especially the performance of holmium devices is presented. The properties of laser planar waveguides obtained by the LPE process and the growth conditions of rare earths doped YAG layers are presented. In this paper we present also the theoretical study of the nonlinear operation of planar waveguide laser, as an example the microdisk Nd:YAG structure is discussed. We derived an approximate formula which relates the small signal gain in the Nd:YAG active medium and the laser characteristics, obtained for whispering-gallery modes and radial modes, to the output power and real parameters of the laser structure

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Authors and Affiliations

W. Woliński
M. Malinowski
A. Mossakowska-Wyszyńska
R. Piramidowicz
P. Szczepański
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Abstract

For many years, a digital waveguide model is being used for sound propagation in the modeling of the vocal tract with the structured and uniform mesh of scattering junctions connected by same delay lines. There are many varieties in the formation and layouts of the mesh grid called topologies. Current novel work has been dedicated to the mesh of two-dimensional digital waveguide models of sound propagation in the vocal tract with the structured and non-uniform rectilinear grid in orientation. In this work, there are two types of delay lines: one is called a smaller-delay line and other is called a larger-delay line. The larger-delay lines are the double of the smaller delay lines. The scheme of using the combination of both smaller- and larger-delay lines generates the non-uniform rectilinear two-dimensional waveguide mesh. The advantage of this approach is the ability to get a transfer function without fractional delay. This eliminates the need to get interpolation for the approximation of fractional delay and give efficient simulation for sound wave propagation in the two-dimensional waveguide modeling of the vocal tract. The simulation has been performed by considering the vowels /ɔ/, /a/, /i/ and /u/ in this work. By keeping the same sampling frequency, the standard two-dimensional waveguide model with uniform mesh is considered as our benchmark model. The results and efficiency of the proposed model have compared with our benchmark model.

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Authors and Affiliations

Tahir Mushtaq Qureshi
Khalid Saifullah Syed
Asim Zafar
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Abstract

A vocal tract model based on a digital waveguide is presented in which the vocal tract has been decomposed into uniform cylindrical segments of variable lengths. We present a model for the real-time numerical solution of the digital waveguide equations in a uniform tube with the temporally varying cross section. In the current work, the uniform cylindrical segments of the vocal tract may have their different lengths, the time taken by the sound wave to propagate through a cylindrical segment in an axial direction may not be an integer multiple of each other. In such a case, the delay in an axial direction is necessarily a fractional delay. For the approximation of fractional-delay filters, Lagrange interpolation is used in the current model. Variable length of the individual segment of the vocal tract enables the model to produce realistic results. These results are validated with accurate benchmark model. The proposed model has been devised to elongate or shorten any arbitrary cylindrical segment by a suitable scaling factor. This model has a single algorithm and there is no need to make section of segments for elongation or shortening of the intermediate segments. The proposed model is about 23% more efficient than the previous model.

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Authors and Affiliations

Tahir Mushtaq Qureshi
Muhammad Ishaq
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Abstract

In cyclic articles previously published we described and analysed self-organized light fibres inside a liquid crystalline (LC) cell contained photosensitive polymer (PP) layer. Such asymmetric LC cell we call a hybrid LC cell. Light fibre arises along a laser beam path directed in plane of an LC cell. It means that a laser beam is parallel to photosensitive layer. We observed the asymmetric LC cell response on an external driving field polarization. Observation has been done for an AC field first. It is the reason we decided to carry out a detailed research for a DC driving field to obtain an LC cell response step by step. The properly prepared LC cell has been built with an isolating layer and garbage ions deletion. We proved by means of a physical model, as well as a numerical simulation that LC asymmetric response strongly depends on junction barriers between PP and LC layers. New parametric model for a junction barrier on PP/LC boundary has been proposed. Such model is very useful because of lack of proper conductivity and charge carriers of band structure data on LC material.

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Authors and Affiliations

P. Moszczyński
A. Walczak
P. Marciniak
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Abstract

We experimentally studied three different D-shape polymer optical fibres with an exposed core for their applications as surface plasmon resonance sensors. The first one was a conventional D-shape fibre with no microstructure while in two others the fibre core was surrounded by two rings of air holes. In one of the microstructured fibres we introduced special absorbing inclusions placed outside the microstructure to attenuate leaky modes. We compared the performance of the surface plasmon resonance sensors based on the three fibres. We showed that the fibre bending enhances the resonance in all investigated fibres. The measured sensitivity of about 610 nm/RIUfor the refractive index of glycerol solution around 1.350 is similar in all fabricated sensors. However, the spectral width of the resonance curve is significantly lower for the fibre with inclusions suppressing the leaky modes.

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Authors and Affiliations

K. Gasior
T. Martynkien
G. Wojcik
P. Mergo
W. Urbanczyk
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Abstract

We experimentally studied three different D-shape polymer optical fibres with an exposed core for their applications as surface plasmon resonance sensors. The first one was a conventional D-shape fibre with no microstructure while in two others the fibre core was surrounded by two rings of air holes. In one of the microstructured fibres we introduced special absorbing inclusions placed outside the microstructure to attenuate leaky modes. We compared the performance of the surface plasmon resonance sensors based on the three fibres. We showed that the fibre bending enhances the resonance in all investigated fibres. The measured sensitivity of about 610 nm/RIU for the refractive index of glycerol solution around 1.350 is similar in all fabricated sensors. However, the spectral width of the resonance curve is significantly lower for the fibre with inclusions suppressing the leaky modes.

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Authors and Affiliations

K. Gasior
T. Martynkien
G. Wojcik
P. Mergo
W. Urbanczyk
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Abstract

Simulation of wave propagation in the three-dimensional (3D) modeling of the vocal tract has shown significant promise for enhancing the accuracy of speech production. Recent 3D waveguide models of the vocal tract have been designed for better accuracy but require a lot of computational tasks. A high computational cost in these models leads to novel work in reducing the computational cost while retaining accuracy and performance. In the current work, we divide the geometry of the vocal tract into four equal symmetric parts with the introduction of two axial perpendicular planes, and the simulation is performed on only one part. A novel strategy is defined to implement symmetric conditions in the mesh. The complete standard 3D digital waveguide model is assumed as a benchmark model. The proposed model is compared with the benchmark model in terms of formant frequencies and efficiency. For the demonstration, the vowels /O/, /i/, /E/, /A/, and /u/ have been selected for the simulations. According to the results, the benchmark and current models are nearly identical in terms of frequency profiles and formant frequencies. Still the current model is three times more effective than the benchmark model.
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Authors and Affiliations

Tahir Mushtaq
1
Ahmad Kamran
1
Muhammad Zubair Akbar Qureshi
2
Zafar Iqbal
3

  1. Department of Mathematics, COMSATS University Islamabad, Vehari Campus, Vehari, Pakistan
  2. Department of Mathematics, Air University, Islamabad, Pakistan
  3. Department of Mathematics, Government Graduate College of Science, Multan, Pakistan
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Abstract

In this paper, a 2D numerical modeling of sound wave propagation in a shallow water medium that acts as a waveguide, are presented. This modeling is based on the method of characteristic which is not constrained by the Courant–Friedrichs–Lewy (CFL) condition. Using this method, the Euler time-dependent equations have been solved under adiabatic conditions inside of a shallow water waveguide which is consists of one homogeneous environment of water over a rigid bed. In this work, the stability and precision of the method of characteristics (MOC) technique for sound wave propagation in a waveguide were illustrated when it was applied with the semi-Lagrange method. The results show a significant advantage of the method of characteristics over the finite difference time domain (FDTD) method.
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Authors and Affiliations

Mohammad Reza Khalilabadi
1

  1. Faculty of Naval Aviation, Malek Ashtar University of Technology, Iran
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Abstract

An optimal design of a slot waveguide is presented for realizing an ultrafast optical modulator based on a 220 nm silicon wafer technology. The recipe is to maximize the confinement and interaction between optical power supported by the waveguide and electric field applied through metallic electrodes. As height of waveguide is fixed at 220 nm, the waveguide and slot width are optimized to maximize the confinement factor of optical power. Moreover, metal electrodes tend to make the waveguide lossy, their optimal placement is calculated to reduce the optical loss and enhance the voltage per unit width in the slot. Performance of an optimally designed slot waveguide with metal electrodes as ultrafast modulator is also discussed.

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Authors and Affiliations

N. Malviya
V. Priye
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Abstract

Adopting mode division multiplex (MDM) technology as the next frontier for optical fiber communication and on-chip optical interconnection systems is becoming very promising because of those remarkable experimental results based on MDM technology to enhance capacity of optical transmission and, hence, making MDM technology an attractive research field. Consequently, in recent years the large number of new optical devices used to control modes, for example, mode converters, mode filters, mode (de)multiplexers, and mode-selective switches, have been developed for MDM applications. This paper presents a review on the recent advances on mode converters, a key component usually used to convert a fundamental mode into a selected high-order mode, and vice versa, at the transmitting and receiving ends in the MDM transmission system. This review focuses on the mode converters based on planar lightwave circuit (PLC) technology and various PLC-based mode converters applied to the above two systems and realized with different materials, structures, and technologies. The basic principles and performances of these mode converters are summarized.
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Bibliography

  1. Essiambre, R. -J., Kramer, G., Winzer, P. J., Foschini, G. J. & Goebel, B. Capacity limits of optical fiber networks. J. Lightwave Technol. 28, 662–701 (2010). https://doi.org/10.1109/JLT.2009.2039464
  2. CISCO: Cisco Visual Netwroking Index: Forecast and Trends, 2017–2022 White Paper.
  3. [Online]. Available at: https://www.cisco.com/c/en/us/solutions/collateral/service-provider/visual-networking-index-vni/white-paper-c11-741490.html. (Accessed: 19th September 2020)
  4. Agrell, E. et al. Roadmap of optical communications. J. Opt. 18, 063002 (2016). http://dx.doi.org/10.1088/2040-8978/18/6/063002
  5. Tkach, R. W. Scaling optical communications for the next decade and beyond. Bell Labs Tech. J. 14, 3–10 (2010). https://doi.org/10.1002/bltj.20400
  6. Yu, J. & Zhang, J. Recent progress on high-speed optical transmission. Digit. Commun. Netw. 2, 65–76 (2016). http://doi.org/10.1016/j.dcan.2016.03.002
  7. Abbas, H. S. & Gregory, M. A. The next generation of passive optical networks: A review. J. Netw. Comput. Appl. 67, 53–74 (2016). http://dx.doi.org/10.1016/j.jnca.2016.02.015
  8. Sillard, P. Next-generation fibers for space-division-multiplexed transmissions. J. Lightwave Technol. 33, 1092–1099 (2015). https://doi.org/10.1109/JLT.2014.2371134
  9. Richardson, D., Fini, J. & Nelson, L. E. Space-division multiplexing in optical fibres. Nat. Photonics 7, 354–362 (2013). https://doi.org/10.1038/nphoton.2013.94
  10. Klaus, W. et al. Advanced space division multiplexing technologies for optical networks. J. Opt. Commun. Netw. 9, C1–C11 (2017). https://doi.org/10.1364/JOCN.9.0000C1
  11. Nakazawa, M. Exabit optical communication explored using 3M scheme. Jap. J. Appl. Phys. 53, , 08MA01 (2014). http://dx.doi.org/10.7567/JJAP.53.08MA01
  12. Winzer, P. J. Optical networking beyond WDM. IEEE Photonics J. 4, 647–651 (2012). https://doi.org/10.1109/JPHOT.2012.2189379
  13. Chiang, K. S. Polymer optical waveguide devices for mode-division-multiplexing applications. Proc. SPIE 10242, Integrated Optics: Physics and Simulations III, 102420R (2017). https://doi.org/10.1117/12.2265275
  14. Sabitu, R., Khan, N. & Malekmohammadi, A. Recent progress in optical devices for mode division multiplex transmission system. Opto-Electron. Review 27, 252–267 (2019). https://doi.org/10.1016/j.opelre.2019.07.001
  15. Ryf, R., Fontaine, N. K., Guan, B., Huang, B. & Tkach, R. W. 305-km combined wavelength and mode-multiplexed transmission over conventional graded-index multimode fibre. in The European Conference on Optical Communication (ECOC), 1–3 (2014).
  16. Hayashi, T. et al. Six-mode 19-core fiber with 114 spatial modes for weakly-coupled mode-division-multiplexed transmission. J. Lightwave Technol. 35, 748–754 (2017). https://doi.org/10.1109/JLT.2016.2617894
  17. Soma, D. et al. 10.16-Peta-B/s dense SDM/WDM transmission over 6-mode 19-core fiber across the C+ L band. J. Lightwave Technol. 36, 1362–1368 (2018). https://doi.org/10.1364/JLT.36.001362
  18. Van Uden, R. et al. Ultra-high-density spatial division multiplexing with a few-mode multicore fibre. Nat. Photon. 8, 865–870 (2014). https://doi.org/10.1038/nphoton.2014.243
  19. Dai, D. X. & Bowers, J. E. Silicon-based on-chip multiplexing technologies and devices for Peta-bit optical interconnects. Nanophotonics 3, 283–311 (2014). https://doi.org/10.1515/nanoph-2013-0021
  20. Luo, L. -W. et al. WDM-compatible mode-division multiplexing on a silicon chip. Nat. Commun. 5, 1–7 (2014). https://doi.org/10.1038/ncomms4069
  21. Hsu, Y. et al. 2.6 Tbit/s on-chip optical interconnect supporting mode-division-multiplexing and PAM-4 signal. IEEE Photonics Technol. Lett. 30, 1052–1055 (2018). https://doi.org/10.1109/LPT.2018.2829508
  22. Zhang, W., Ghorbani, H., Shao, T. & Yao, J. On-Chip 4×10 GBaud/s Mode-Division Multiplexed PAM-4 Signal Transmission. IEEE J. Sel. Top. Quantum Electron. 26, 1–8 (2020). https://doi.org/10.1109/JSTQE.2020.2964388
  23. Huang, Y., Xu, G. & Ho, S. -T. An ultracompact optical mode order converter. IEEE Photonics Technol. Lett. 18, 2281–2283 (2006). https://doi.org/10.1109/LPT.2006.884886
  24. Oner, B., Üstün, K., Kurt, H., Okyay, A. K. & Turhan-Sayan, G. Large bandwidth mode order converter by differential waveguides. Opt. Express 23, 3186–3195 (2015). https://doi.org/10.1364/OE.23.003186
  25. Uematsu, T., Ishizaka, Y., Kawaguchi, Y., Saitoh, K. & Koshiba, M. Design of a compact two-mode multi/demultiplexer consisting of multimode interference waveguides and a wavelength-insensitive phase shifter for mode-division multiplexing transmission. J. Lightwave Technol. 30, 2421–2426 (2012). https://doi.org/10.1109/JLT.2012.2199961
  26. Han, L., Liang, S., Zhu, H., Qiao, L., Xu, J. & Wang, W. Two-mode de/multiplexer based on multimode interference couplers with a tilted joint as phase shifter. Opt. Lett. 40, 518-521 (2015). http://dx.doi.org/10.1364/OL.40.000518
  27. Guo, F. et al. An MMI-based mode (DE) MUX by varying the waveguide thickness of the phase shifter. IEEE Photonics Technol. Lett. 28, 2443–2446 (2016). https://doi.org/10.1109/LPT.2016.2599934
  28. Chack, D., Hassan, S. & Qasim, M. Broadband and low crosstalk silicon on-chip mode converter and demultiplexer for mode division multiplexing. Appl. Opt. 59, 3652–3659 (2020). https://doi.org/10.1364/AO.390085
  29. Linh, H. D. T., Dung, T. C., Tanizawa, K., Thang, D. D. & Hung, N. T. Arbitrary TE0/TE1/TE2/TE3 Mode Converter Using 1× 4 Y-Junction and 4× 4 MMI Couplers. IEEE J. Sel. Top. Quantum Electron. 26, 1–8 (2019). https://doi.org/10.1109/JSTQE.2019.2937169
  30. González-Andrade, D. et al. Ultra-broadband mode converter and multiplexer based on sub-wavelength structures. IEEE Photonics J. 10, 1–10 (2018). https://doi.org/10.1109/JPHOT.2018.2819364
  31. Leuthold, J., Eckner, J., Gamper, E., Besse, P. A. & Melchior, H. Multimode interference couplers for the conversion and combining of Zero- and First-Order modes. J. Lightwave Technol. 16, 1228–1239 (1998). https://doi.org/10.1109/50.701401
  32. Guo, F. et al.Two-mode converters at 1.3 μm based on multimode interference couplers on InP substrates. Chin. Phys. Lett. 33, 024203 (2016). http://dx.doi.org/10.1088/0256-307X/33/2/024203
  33. Chen, H. -T. & Webb, K. J. Silicon-on-insulator irregular waveguide mode converters. Opt. Lett. 31, 2145–2147 (2006). https://doi.org/10.1364/OL.31.002145
  34. Chen, D. et al. Low-loss and fabrication tolerant silicon mode-order converters based on novel compact tapers. Opt. Express 23, 11152–11159 (2015). https://doi.org/10.1364/OE.23.011152
  35. Chen, Z. Y. Bridged coupler and oval mode converter based silicon mode division (de)multiplexer and Terabit WDM-MDM system demonstration. J. Lightwave Technol. 36, 2757–2766 (2018). https://dx.doi.org/10.1109/JLT.2018.2818793
  36. Zhu, D. et al. Design of compact TE-polarized mode-order converter in silicon waveguide with high refractive index material. IEEE Photonics J. 10, 1–7 (2018). https://doi.org/10.1109/JPHOT.2018.2883209
  37. Abu-Elmaaty, B. E., Sayed, M. S., Pokharel, R. K. & Shalaby, H. M. General silicon-on-insulator higher-order mode converter based on substrip dielectric waveguides. Appl. Opt. 58, 1763–1771 (2019). https://doi.org/10.1364/AO.58.001763
  38. Cheng, Z. et al. Sub-wavelength grating assisted mode order converter on the SOI substrate. Opt. Express 27, 34434–34441 (2019). https://doi.org/10.1364/OE.27.034434
  39. Ye, W., Yuan, X., Gao, Y. & Liu, J. Design of broadband silicon-waveguide mode-order converter and polarization rotator with small footprints. Opt. Express 25, 33176–33183 (2017). https://doi.org/10.1364/OE.25.033176
  40. Liu, L. et al. Design of a compact silicon-based TM-polarized mode-order converter based on shallowly etched structures. Appl. Opt. 58, 9075–9081 (2019). https://doi.org/10.1364/AO.58.009075
  41. Hao, L. et al. Efficient TE-polarized mode-order converter based on high-index-contrast polygonal slot in a silicon-on-insulator waveguide. IEEE Photonics J. 11, 1–10 (2019). https://doi.org/10.1109/JPHOT.2019.2907640
  42. Zhao, Y. et al. Ultra-compact silicon mode-order converters based on dielectric slots. Opt. Lett. 45, 3797–3800 (2020). https://doi.org/10.1364/OL.391748
  43. Jia, H. et al. Ultra-compact dual-polarization silicon mode-order converter. Opt. Lett. 44, 4179–4182 (2019). https://doi.org/10.1364/OL.44.004179
  44. Zhang, M. R., Chen, K. X., Jin, W. & Chiang, K. S. Electro-optic mode switch based on lithium-niobate Mach–Zehnder interferometer. Appl. Opt. 55, 4418–4422 (2016). https://doi.org/10.1364/AO.55.004418
  45. Hanzawa, N. et al. Two-mode PLC-based mode multi/demultiplexer for mode and wavelength division multiplexed transmission. Opt. Express 21, 25752–25760 (2013). https://doi.org/10.1364/OE.21.025752
  46. Saitoh, K. et al. PLC-based LP11 mode rotator for mode-division multiplexing transmission. Opt. Express 22, 19117–19130 (2014). https://doi.org/10.1364/OE.22.019117
  47. Hanzawa, N. et al. Mode multi/demultiplexing with parallel waveguide for mode division multiplexed transmission. Opt. Express 22, 29321–29329 (2014). https://doi.org/10.1364/OE.22.029321
  48. Hanzawa, N. et al. PLC-based four-mode multi/demultiplexer with LP11 mode rotator on one chip. J. Lightwave Technol. 33, 1161–1165 (2015). https://doi.org/10.1109/JLT.2014.2378281
  49. Saitoh, K. et al. PLC-based mode multi/demultiplexers for mode division multiplexing. Opt. Fiber Technol. 35, 80–92 (2017). https://doi.org/10.1016/j.yofte.2016.08.002
  50. Riesen, N., Gross, S., Love, J. D. & Withford, M. J. Femtosecond direct-written integrated mode couplers. Opt. Express 22, 29855–29861 (2014). https://doi.org/10.1364/OE.22.029855
  51. Dong, J. L., Chiang, K. S. & Jin, W. Compact three-dimensional polymer waveguide mode multiplexer. J. Lightwave Technol. 33, 4580–4588 (2015). https://doi.org/10.1109/JLT.2015.2478961
  52. Wei, F. K., Chen, K. X. & Chiang, K. S. Mode conversion with vertical polymer-waveguide directional coupler. in Asia Communication and Photonics Conference, AF1G.3 (2016). https://doi.org/10.1364/ACPC.2016.AF1G.3
  53. Huang, Q. D., Wu, Y. F., Jin, W. & Chiang, K. S. Mode multiplexer with cascaded vertical asymmetric waveguide directional couplers. J. Lightwave Technol. 36, 2903–2911 (2018). https://dx.doi.org/10.1109/JLT.2018.2829143
  54. Zhao, W. K., Chen, K. X., Wu, J. Y. & Chiang, K. S. Horizontal directional coupler formed with waveguides of different heights for mode-division multiplexing. IEEE Photonics J. 9, 1–9 (2017). https://doi.org/10.1109/JPHOT.2017.2731046
  55. Zhao, W. K., Chen, K. X. & Wu, J. Y. Broadband mode multiplexer formed with non-planar tapered directional couplers. IEEE Photonics Technol. Lett. 31, 169–172 (2018). https://doi.org/10.1109/LPT.2018.2887352
  56. Yin, M., Deng, Q., Li, Y., Wang, X. & Li, H. Compact and broadband mode multiplexer and demultiplexer based on asymmetric plasmonic–dielectric coupling. Appl. Opt. 53, 6175–6180 (2014). https://doi.org/10.1364/AO.53.006175
  57. Wang, J., Chen, P., Chen, S., Shi, Y. & Dai, D. X. Improved 8-channel silicon mode demultiplexer with grating polarizers. Opt. Express 22, 12799–12807 (2014). https://doi.org/10.1364/OE.22.012799
  58. Garcia-Rodriguez, D., Corral, J. L. Griol, A. & Llorente, R. Dimensional variation tolerant mode converter/multiplexer fabricated in SOI technology for two-mode transmission at 1550 nm. Opt. Lett. 42, 1221–1224 (2017). https://doi.org/10.1364/OL.42.001221
  59. Luo, L. -W., Gabrielli, L. H. & Lipson, M. On-chip mode-division multiplexer. in Conference on Lasers and Electro-Optics (CLEO 2013) CTh1C.6. (2013). https://doi.org/10.1364/CLEO_SI.2013. CTh1C.6
  60. Yu, Y., Ye, M. & Fu, S. On-chip polarization controlled mode converter with capability of WDM operation. IEEE Photonics Technol. Lett. 27, 1957–1960 (2015). https://doi.org/10.1109/LPT.2015.2448076
  61. Yang, Y., Chen, K. X., Jin, W. & Chiang, K. S. Widely wavelength-tunable mode converter based on polymer waveguide grating. IEEE Photonics Technol. Lett. 27, 1985–1988 (2015). https://doi.org/10.1109/LPT.2015.2448793
  62. Jin, W. & Chiang, K. S. Mode converter with sidewall-corrugated polymer waveguide grating. in Opto-Electronics Communication Conference (OECC2015), 1–3 (2015). https://doi.org/10.1109/OECC.2015.7340081
  63. Jin, W. & Chiang, K. S. Mode converters based on cascaded long-period waveguide gratings. Opt. Lett. 41, 3130–3133 (2016). https://doi.org/10.1364/OL.41.003130
  64. Wang, W., Wu, J. Y., Chen, K. X., Jin, W. & Chiang, K. S. Ultra-broadband mode converters based on length-apodized long-period waveguide gratings. Opt. Express 25, 14341–14350 (2017). https://doi.org/10.1364/OE.25.014341
  65. Zhao, W. K., Chen, K. X. & Wu, J. Y. Ultra-short embedded long-period waveguide grating for broadband mode conversion. App. Phys. B 125, 177 (2019). https://doi.org/10.1007/s00340-019-7290-0
  66. Jin, W. & Chiang, K. S. Three-dimensional long-period waveguide gratings for mode-division-multiplexing applications. Opt. Express 26, 15289–15299 (2018). https://doi.org/10.1364/OE.26.015289
  67. Castro, J. M. et al. Demonstration of mode conversion using anti-symmetric waveguide Bragg gratings. Opt. Express 13, 4180–4184 (2005). https://doi.org/10.1364/OPEX.13.004180
  68. Xiao, R. et al. On-chip mode converter based on two cascaded Bragg gratings. Opt. Express 27, 1941–1957 (2019). https://doi.org/10.1364/OE.27.001941
  69. Wang, H. et al. Compact silicon waveguide mode converter employing dielectric metasurface structure. Adv. Opt. Mater. 7, 1801191 (2019). https://doi.org/10.1002/adom.201801191
  70. Ohana, D. & Levy, U. Mode conversion based on dielectric metamaterial in silicon. Opt. Express 22, 27617–27631 (2014). https://doi.org/10.1364/OE.22.027617
  71. Ohana, D., Desiatov, B., Mazurski, N. & Levy, U. Dielectric metasurface as a platform for spatial mode conversion in nanoscale waveguides. Nano Lett. 16, 7956–7961 (2016). https://doi.org/10.1021/acs.nanolett.6b04264
  72. Qiu, H. et al. Silicon mode multi/demultiplexer based on multimode grating-assisted couplers. Opt. Express 21, 17904–17911 (2013). https://doi.org/10.1364/OE.21.017904
  73. Zhao, W. K., Feng, J., Chen, K. X. & Chiang, K. S. Reconfigurable broadband mode (de) multiplexer based on an integrated thermally induced long-period grating and asymmetric Y-junction. Opt. Lett. 43, 2082–2085 (2018). https://doi.org/10.1364/OL.43.002082
  74. Zi, X. Z., Wang, L. F., Chen, K. X. & Chiang, K. S. Mode-selective switch based on thermo-optic asymmetric directional coupler. IEEE Photonics Technol. Lett. 30, 618–621 (2018). https://doi.org/10.1109/LPT.2018.2808466
  75. Jin, W. & Chiang, K. S. Mode switch based on electro-optic long-period waveguide grating in lithium niobate. Opt. Lett. 40, 237–240 (2015). https://doi.org/10.1364/OL.40.000237
  76. Jin, W. & Chiang, K. S. Reconfigurable three-mode converter based on cascaded electro-optic long-period gratings. IEEE J. Sel. Top. Quantum Electron. 26, 1–6 (2020). https://doi.org/10.1109/JSTQE.2020.2969568
  77. Zhang, M. R., Ai, W., Chen, K. X., Jin, W. & Chiang, K. S. A lithium-niobate waveguide directional coupler for switchable mode multiplexing. IEEE Photonics Technol. Lett. 30, 1764–1767 (2018). https://doi.org/10.1109/LPT.2018.2868834
  78. Lee, B. -T. & Shin, S. -Y. Mode-order converter in a multimode waveguide. Opt. Lett. 28, 1660–1662 (2003). https://doi.org/10.1364/OL.28.001660
  79. Low, A. L., Yong, Y. S., You, A. H., Chien, S. F. & Teo, C. F. A five-order mode converter for multimode waveguide. IEEE Photonics Technol. Lett. 16, 1673–1675 (2004). https://doi.org/10.1109/LPT.2004.828512
  80. Riesen, N. & Love, J. D. Design of mode-sorting asymmetric Y-junctions. App. Opt. 51, 2778–2783 (2012). https://doi.org/10.1364/AO.51.002778
  81. Driscoll, J. B. et al. .Asymmetric Y junctions in silicon waveguides for on-chip mode-division multiplexing. Opt. Lett. 38, 1854–1856 (2013). https://doi.org/10.1364/OL.38.001854
  82. Feng, J., Chen, K. X., Ren, K. Y. & Chiang, K. S. Mode (de) multiplexer based on polymer-waveguide asymmetric Y-junction. in Asia Communication and Photonics Conference AF1G.5 (2016). https://doi.org/10.1364/ACPC.2016.AF1G.5
  83. Chen, W. W. et al. Silicon three-mode (de)multiplexer based on cascaded asymmetric Y junctions. Opt. Lett. 41, 2851–2854 (2016). https://doi.org/10.1364/OL.41.002851
  84. Fujisawa, T. et al. Scrambling-type three-mode PLC multiplexer based on cascaded Y-branch waveguide with integrated mode rotator. J. Lightwave Technol. 36, 1985–1992 (2018). https://doi.org/10.1109/JLT.2018.2798619
  85. Gao, Y. et al. Compact six-mode (de) multiplexer based on cascaded asymmetric Y-junctions with mode rotators. Opt. Commun. 451, 41–45 (2019). https://dx.doi.org/10.1016/j.optcom.2019.06.010
  86. Watanabe, T. & Kokubun, Y. Demonstration of mode-evolutional multiplexer for few-mode fibers using stacked polymer waveguide. IEEE Photonics J. 7, 1–11 (2015). https://doi.org/10.1109/JPHOT.2015.2497234
  87. Dai, D. X., Tang, Y. B. & Bowers, J. E. Mode conversion in tapered submicron silicon ridge optical waveguides. Opt. Express 20, 13425–13439 (2012). https://doi.org/10.1364/OE.20.013425
  88. Dai, D. X. & Mao, M. Mode converter based on an inverse taper for multimode silicon Nanophotonicsic integrated circuits Opt. Express 23, 28376–28388 (2015). https://doi.org/10.1364/OE.23.028376
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Authors and Affiliations

Areez K. Memon
1
Kai X. Chen
1

  1. School of Optoelectronic Science and Engineering, University of Electronic Science and Technology of China, Chengdu 610054, P.R. China
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Abstract

In this article, we propose the realization of XNOR logic function by using all-optical XOR and NOT logic gates. Initially, both XOR and NOT gates are designed, simulated and optimized for high contrast outputs. T-shaped waveguides are created on the photonic crystal platform to realize these logic gates. An extra input is used to perform the inversion operation in the NOT gate. Inputs in both the gates are applied with out of phase so as to have a destructive interference between them and produce negligible intensity for logic ‘0'. The XOR and NOT gates are simulated using Finite Difference Time Domain method which results with a high contrast ratio of 55.23 dB and 54.83 dB, respectively at a response time of 0.136 ps and 0.1256 ps. Later, both the gates are cascaded by superimposing the output branch of the waveguide of XOR gate with the input branch of the waveguide of NOT gate so that it can be resulted with compact size for XNOR logic function. The resultant structure of XNOR logic came out with the contrast ratio of 12.27 dB at a response time of 0.1588 ps. Finally, it can be concluded that the proposed structures with fair output performance can suitably be applied in the design of photonic integrated circuits for high speed computing and telecommunication systems.

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Authors and Affiliations

E.H. Shaik
N. Rangaswamy
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Abstract

This paper presents how to design and simulate two different topologies of a bandpass (BP) rectangular waveguide filter using a direct coupled resonator technique operating at 12 GHz. The filters are characterized by a cross coupling (CM) which produces a single attenuation pole at finite frequency used to realize the bandpass response. The filter resonators provide3rd and 4th order designs with a pseudoelliptic response using High Frequency Structure Simulator (HFSS) simulator. Transmission zeros are obtained through coupling between the fundamental mode and high mode. The filter structures are validated leading to obtain transmission zeros close to the bandpass. The simulated waveguide filters with a central frequency exhibit an insertion loss of 0.4/0.3dB and a return loss of 20/23dB for the whole bandwidth ranging from 11.85GHz to 12.15GHz that show good electromagnetic responses for the simulated rectangular waveguide filters.
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Authors and Affiliations

Gouni Slimane
1
Damou Mehdi
Chetioui Mohammed
2
Boudkhil Abdelhakim
2

  1. Laboratory of Electronics, Signal Processing and Microwave and Laboratory Technology of Communication, Faculty of Technology University Tahar Moulay of Saida, Algeria
  2. Laboratory of Telecommunications, Abu Bakr Belkaid University of Tlemcen, Algeria
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Abstract

The paper presents the concept of a fully planar treeshaped antenna with quasi-fractal geometry. The shape of the proposed radiator is based on a multi-resonant structure. Developed planar tree has symmetrical branches with different length and is fed by a coplanar waveguide (CPW) with modified edge of the ground plane. The antenna of size 29 mm x25 mm has been designed on Taconic - RF-35 substrate (r = 3.5, tg= 0.0018, h = 0.762 mm). The paper shows simulated and measured characteristics of return loss, as well as measured radiation patterns. The proposed antenna could be a good candidate for broadband applications (for instance: wideband imaging for medical application and weather monitoring radars in satellite communication etc.)

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Authors and Affiliations

Małgorzata Malinowska
Marek Kitliński
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Abstract

Network on chip (NoC) is presented as a promising solution to face off the growing up of the data exchange in the multiprocessor system-on-chip (MPSoC). However, the traditional NoC faces two main problems: the bandwidth and the energy consumption. To face off these problems, a new technology in MPSoC, namely, optical network-on-chip (ONoC) has been introduced which it uses the optical communication to guaranty a high performance in communication between cores. In addition, wavelength division multiplexing (WDM) is exploited in ONoC to reach a high rate of bandwidth. Nevertheless, the transparency nature of the ONoC components induce crosstalk noise to the optical signals, which it has a direct effect to the signal-to-noise ratio (SNR) then decrease the performance of the ONoC. In this paper, we proposed a new system to control these impairments in the network in order to detect and monitor crosstalk noise in WDM-based ONoC. Furthermore, the crosstalk monitoring system is a distributed hardware system designed and test with the different optical components according the various network topology used in ONoC. The register-transfer level (RTL) hardware design and implementation of this system can result in high reliability, scalability and efficiency with running time less than 20 ms.

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Authors and Affiliations

Ahmed Jedidi
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Abstract

Fano resonance is an optical effect that emerges from the coherent coupling and interference (constructive and destructive) between the continuous state (background process) and the Lorentzian state (resonant process) in the plasmonic waveguide-resonator system. This effect has been used in the applications like optical sensors. These sensors are extensively used in sensing biochemicals and gases by the measurement of refractive index changes as they offer high sensitivity and ultra-high figure of merit. Herein, we surveyed several plasmonic Fano sensors with different geometries composed of metal-insulator-metal waveguide(s). First, the resonators are categorized based on different architectures. The materials and methods adopted for these designs are precisely surveyed and presented. The performances are compared depending upon the characterization parameters like sensitivity and figure of merit. Finally, based on the survey of very recent models, the advances and challenges of refractive index sensing deployed on Fano resonances are discussed.
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Bibliography

  1. De Tommasi, E. et al. Frontiers of light manipulation in natural, metallic, and dielectric nanostructures. Riv. del Nuovo Cim. 44, 1–68 (2021). https://doi.org/10.1007/s40766-021-00015-w
  2. Maier, S. Surface plasmon polaritons at metal /insulator interfaces. in Plasmonics: Fundamentals and Applications:Chapter 2, 1–2 (Springer, New York, 2007). https://doi.org/10.1007/0-387-37825-1_2
  3. Zhang, J., Zhang, L. & Xu, W. Surface plasmon polaritons: Physics and applications. J. Phys. D. Appl. Phys. 45, 113001 (2012).span> https://doi.org/10.1088/0022-3727/45/11/113001
  4. Naik, G. V, Shalaev, V. M. & Boltasseva, A. Alternative plasmonic materials: beyond gold and silver. Adv. Mater. 25, 3264–3294 (2013). https://doi.org/10.1002/adma.201205076
  5. Luo, & Yan, L. Surface plasmon polaritons and its applications. IEEE Photon. J. 4, 590–595 (2012). https://doi.org/10.1109/JPHOT.2012.2189436.
  6. Saleh, E. A. & Teich, M. C. Fundamentals of Photonics. 1114–1115 (2nd ed.) (Wiley press, 2007). https://doi.org/10.1063/1.2809878
  7. Gramotnev, K. & Bozhevolnyi, S. I. Plasmonics beyond the diffraction limit. Nat. Photonics 4, 83–91 (2010). https://doi.org/10.1038/nphoton.2009.282
  8. Kinsey, N., Ferrera, M., Shalaev, V. M. & Boltasseva, A. Examining nanophotonics for integrated hybrid systems: a review of plasmonic interconnects and modulators using traditional and alternative materials [Invited]. Opt. Soc. Am. B 32, 121–142 (2015). https://doi.org/10.1364/JOSAB.32.000121
  9. Amoosoltani, N., Yasrebi, N., Farmani, A. & Zarifkar, A. A plasmonic nano-biosensor based on two consecutive disk resonators and unidirectional reflectionless propagation IEEE Sens. J. 20, 9097–9104 (2020). https://doi.org/10.1109/JSEN.2020.2987319
  10. Han, Z. & Bozhevolnyi, S. I. Radiation guiding with surface plasmon polaritons. Reports Prog. Phys. 76, 016402 (2013). https://doi.org/10.1088/0034-4885/76/1/016402
  11. Lu, H., Wang, G. X. & Liu, X.M. Manipulation of light in MIM plasmonic waveguide systems. Chin. Sci. Bull. 58, 3607–3616 (2013). https://doi.org/10.1007/s11434-013-5989-6
  12. Onbasli, M. C. & Okyay, A. K. Nanoantenna couplers for metal-insulator-metal waveguide interconnects. Proc. SPIE 7757, 77573R (2010). https://doi.org/10.1117/12.876177
  13. Limonov, M. F., Rybin, M. V., Poddubny, A. N. & Kivshar, Y. S. Fano resonances in photonics. Nat. Photonics 11, 543–554 (2017). https://doi.org/10.1038/nphoton.2017.142
  14. Luk’Yanchuk, B. et al. The Fano resonance in plasmonic nanostructures and metamaterials. Nat. Mater. 9, 707–715 (2010). https://doi.org/10.1038/nmat2810
  15. Wang, J. et al. Double Fano resonances due to interplay of electric and magnetic plasmon modes in planar plasmonic structure with high sensing sensitivity. Express 21, 2236–2244 (2013). https://doi.org/10.1364/OE.21.002236
  16. Lovera, A., Gallinet, B., Nordlander, P. & Martin, O. J. F. Mechanisms of Fano resonances in coupled plasmonic systems. ACS Nano 7, 4527–4536 (2013). https://doi.org/10.1021/nn401175j
  17. Fan, J. A. et al. Fano-like interference in self-assembled plasmonic quadrumer clusters. Nano Lett. 10, 4680–4685 (2010) . https://doi.org/10.1021/nl1029732
  18. Kazanskiy, N. L., Khonina, S. N. & Butt, M. A. Plasmonic sensors based on metal-insulator-metal waveguides for refractive index sensing applications: A brief Phys. E Low Dimens. Syst. Nanostruct. 117, 113798 (2020). https://doi.org/10.1016/j.physe.2019.113798
  19. Verellen, N. et al. Mode parity-controlled Fano- and Lorentz-like line shapes arising in plasmonic nanorods. Nano Lett. 14, 2322–2329 (2014). https://doi.org/10.1021/nl404670x
  20. Huang, Y., Min, C., Dastmalchi, P. & Veronis, G. Slow-light enhanced subwavelength plasmonic waveguide refractive index sensors. Opt. Express 23, 14922 (2015) . https://doi.org/10.1364/OE.23.014922
  21. Luo, S., Li, B., Xiong, D., Zuo, D. & Wang, X. A high performance plasmonic sensor based on metal-insulator-metal waveguide coupled with a double-cavity structure. Plasmonics 12, 223–227 (2017). https://doi.org/10.1007/s11468-016-0253-y
  22. Rakhshani, M. R. & Mansouri-Birjandi, M. A. A high-sensitivity sensor based on three-dimensional metal–insulator–metal racetrack resonator and application for hemoglobin Photonics Nanostruct. 32, 28–34 (2018). https://doi.org/10.1016/j.photonics.2018.08.002
  23. Butt, M. A., Khonina, S. N. & Kazanskiy, N. L. Plasmonic refractive index sensor based on metal–insulator-metal waveguides with high sensitivity. J. Mod. Opt. 66, 1038–1043 (2019). https:/doi.org/10.1080/09500340.2019.1601272
  24. Butt, M. A., Khonina, S. N. & Kazanskiy, N. L. An array of nano-dots loaded MIM square ring resonator with enhanced sensitivity at NIR wavelength range. Optik 202, 163655 (2020). https://doi.org/10.1016/j.ijleo.2019.163655
  25. Economou,  N. Surface plasmons in thin films. Phys. Rev. 182, 539–554 (1969). https://doi.org/10.1103/PhysRev.182.539
  26. Yang, & Lu, Z. Subwavelength plasmonic waveguides and plasmonic materials. Int. J. Opt. 2012 (2012). https://doi.org/10.1155/2012/258013
  27. Han, Z. & Bozhevolnyi, S. I. Plasmon-induced transparency with detuned ultracompact Fabry-Perot resonators in integrated plasmonic devices. Opt. Express 19, 3251 (2011). https://doi.org/10.1364/OE.19.003251
  28. Zhan, S. et al. Slow light based on plasmon-induced transparency in dual-ring resonator-coupled MDM waveguide system. J. Phys. D. Appl. Phys. 47, (2014).https:/doi.org/10.1088/0022-3727/47/20/205101
  29. Piao, X., Yu, S., Koo, S., Lee, K. & Park, N. Fano-type spectral asymmetry and its control for plasmonic metal-insulator-metal stub structures. Opt. Express 19, 10907–10912 (2011). https://doi.org/10.1364/OE.19.010907
  30. Fu, Y. H., Zhang, J. B., Yu, Y. F. & Luk’yanchuk, B. Generating and manipulating higher order Fano resonances in dual-disk. ACS Nano 6, 5130–5137 (2012). https://doi.org/10.1021/nn3007898
  31. Fang, J., Zhang, M., Zhang, F. & Yu, H. Plasmonic sensor based on Fano resonance. Guangdian Gongcheng/Opto-Electron. Eng. 44, 221–225 (2017). https://doi.org/10.3969/j.issn.1003-501X.2017.02.012
  32. Yu, Y. et al. Nonreciprocal transmission in a nonlinear photonic-crystal Fano structure with broken symmetry. Laser Photonics Rev. 9, 241–247 (2015). https://doi.org/10.1002/lpor.201400207
  33. Chen, Z. & Yu, L. Multiple Fano resonances based on different waveguide modes in a symmetry breaking plasmonic system. IEEE Photonics J. 6, 1–8 (2014). https://doi.org/ 1109/JPHOT.2014.2368779
  34. Miroshnichenko, A. E., Flach, S. & Kivshar, Y. S. Fano resonances in nanoscale structures. Rev. Mod. Phys. 82, 2257–2298 (2010). https://doi.org/10.1103/RevModPhys.82.2257
  35. Chen, Z. et al. A refractive index nanosensor based on Fano resonance in the plasmonic waveguide system. IEEE Photon. Technol. Lett. 27, 1695–1698 (2015). https://doi.org/ 1109/LPT.2015.2437850
  36. Wei, W., Yan, X., Shen, B. & Zhang, X. Plasmon-induced transparency in an asymmetric bowtie structure. Nanoscale Res. Lett. 14, 246 (2019). https://doi.org/10.1186/s11671-019-3081-0
  37. Song, H., Singh, R., Cong, L. & Yang, H. Engineering the Fano resonance and electromagnetically induced transparency in near-field coupled bright and dark J. Phys. D. Appl. Phys. 48, 035104 (2015). https://doi.org/10.1088/0022-3727/48/3/035104
  38. Yu, S., Piao, X., Hong, J. & Park, N. Progress toward high-Q perfect absorption : A Fano anti-laser. Phys. Rev. A 92, 011802R (2015). https://doi.org/10.1103/PhysRevA.92.011802
  39. Yan, X. et al. High sensitivity nanoplasmonic sensor based on plasmon-induced transparency in a graphene nanoribbon waveguide coupled with detuned graphene square-nanoring Plasmonics 12, 1449–1455 (2016). https://doi.org/10.1007/s11468-016-0405-0
  40. Chen, J., Gan, F., Wang, Y. & Li, G. Plasmonic sensing and modulation based on Fano resonances. Adv. Opt. Mater. 6, 1701152 (2018). https://doi.org/10.1002/adom.201701152
  41. Deng, Y., Cao, G. & Yang, H. Tunable Fano resonance and high-sensitivity sensor with high figure of merit in plasmonic coupled cavities. Photonics Nanostruct. 28, 45–51 (2018). https://doi.org/10.1016/j.photonics.2017.11.008
  42. Hayashi, S., Nesterenko, D. V. & Sekkat, Z. Fano resonance and plasmon-induced transparency in waveguide-coupled surface plasmon resonance sensors. Appl. Express 8, 022201 (2015). https://doi.org/10.7567/apex.8.022201
  43. Heuck, M., Kristensen, P. T., Elesin, Y. & Mørk, J. Improved switching using Fano resonances in photonic crystal structures. Opt. Lett. 38, 2466 (2013). https://doi.org/10.1364/OL.38.002466
  44. Chen, Z. et al. Plasmonic wavelength demultiplexers based on tunable Fano resonance in coupled-resonator systems. Opt. Commun. 320, 6–11 (2014). https://doi.org/10.1016/j.optcom.2013.12.079
  45. Qi, J. et al. Independently tunable double Fano resonances in asymmetric MIM waveguide structure. Opt. Express 22, 14688–14695 (2014). https://doi.org/10.1364/OE.22.014688
  46. Chen, Z.-Q. et al. Fano resonance based on multimode interference in symmetric plasmonic structures and its applications in plasmonic nanosensors. Chin. Lett. 30, 057301 (2013). https://doi.org/10.1088/0256-307x/30/5/057301
  47. Gu, P., Birch, D. J. S. & Chen, Y. Dye-doped polystyrene-coated gold nanorods: Towards wavelength tuneable SPASER. Methods Appl. Fluoresc. 2, 024004 (2014). https://doi.org/10.1088/2050-6120/2/2/024004
  48. Zafar, R. & Salim, M. Enhanced Figure of Merit in Fano resonance-based plasmonic refractive index sensor. IEEE Sens. J. 15, 6313–6317 (2015). https://doi.org/10.1109/JSEN.2015.2455534
  49. Zhang, Y. et al. Evolution of Fano resonance based on symmetric/asymmetric plasmonic waveguide system and its application in nanosensor. Opt. Commun. 370, 203–208 (2016). https://doi.org/10.1016/j.optcom.2016.03.001
  50. Zhang, Y. et al. Ultra-high Sensitivity plasmonic nanosensor based on multiple Fano resonance in the MDM side-coupled cavities. Plasmonics 12, 1099– 1105 (2017). https://doi.org/10.1007/s11468-016-0363-6
  51. Kocabas, S. E., Veronis, G., Miller, D. A. B. & Fan, S. Transmission line and equivalent circuit models for plasmonic waveguide components. EEE J. Sel. Top. Quantum 14, 1462–1472 (2008). https://doi.org/10.1109/JSTQE.2008.924431
  52. Han, Z., Van, V., Herman, W. N. & Ho, P.-T. Aperture-coupled MIM plasmonic ring resonators with sub-diffraction modal volumes. Opt. Express 17, 12678– 12684 (2009). https://doi.org/10.1364/OE.17.012678
  53. Li, Q., Wang, T., Su, Y., Yan, M. & Qiu, M. Coupled mode theory analysis of mode-splitting in coupled cavity system. Opt. Express 18, 8367 (2010). https://doi.org/10.1364/OE.18.008367
  54. Achanta, V.G. Surface waves at metal-dielectric interfaces: Material science perspective. Rev. Phys. 5, 100041 (2020). https://doi.org/10.1016/j.revip.2020.100041
  55. Niu, L., Zhang, J. B., Fu, Y. H., Kulkarni, S. & Luky`anchuk, B. Fano resonance in dual-disk ring plasmonic nanostructures. Opt. Express 19, 22974–22981 (2011). https://doi.org/10.1364/OE.19.022974
  56. Kolwas, K. & Derkachova, A. Impact of the Interband transitions in gold and silver on the dynamics of propagating and localized surface plasmons. Nanomaterials 10, 1411 (2020). https://doi.org/10.3390/nano10071411
  57. Thomas, A. Plasmonics. in Narrow Plasmon Resonances in Hybrid Systems 7–27 (Springer, 2018). https://doi.org/10.1007/978-3-319-97526-9
  58. Noah, N. M. Design and synthesis of nanostructured materials for sensor applications. J. Nanomater. 2020, 8855321 (2020). https://doi.org/10.1155/2020/8855321
  59. Chen, F. & Yao, D. Realizing of plasmon Fano resonance with a metal nanowall moving along MIM waveguide. Opt. Commun. 369, 72–78 (2016). https://doi.org/10.1016/j.optcom.2016.02.024
  60. Zhang, Y. et al. High-sensitivity refractive index sensors based on Fano resonance in the plasmonic system of splitting ring cavity-coupled MIM waveguide with tooth Appl. Phys. A 125, 13 (2019). https://doi.org/10.1007/s00339-018-2283-0
  61. Chen, Y., Xu, Y. & Cao, J. Fano resonance sensing characteristics of MIM waveguide coupled square convex ring resonator with metallic baffle. Results Phys. 14, 102420 (2019). https://doi.org/10.1016/j.rinp.2019.102420
  62. Naik, G. V., Kim, J. & Boltasseva, A. Oxides and nitrides as alternative plasmonic materials in the optical range. Opt. Mater. Express 1, 1090–1099 (2011). https://doi.org/10.1364/OME.1.001090
  63. West, R. et al. Searching for better plasmonic materials. Laser Photonics Rev. 4, 795–808 (2010). https://doi.org/10.1002/lpor.200900055
  64. Deng, Y. et al. Tunable and high-sensitivity sensing based on Fano resonance with coupled plasmonic cavities. Sci. Rep. 7, 10639 (2017). https://doi.org/10.1038/s41598-017-10626-1
  65. Zhang, Z. et al. Plasmonic refractive index sensor with high figure of merit based on concentric-rings resonator. Sensors 18, 116 (2018). https://doi.org/10.3390/s18010116
  66. Chauhan, D., Adhikari, R., Saini, R. K., Chang, S. H. & Dwivedi, R. P. Subwavelength plasmonic liquid sensor using Fano resonance in a ring resonator structure. Optik 223, 165545 (2020). https://doi.org/10.1016/j.ijleo.2020.165545
  67. Zhang, Z., Luo, L., Xue, C., Zhang, W. & Yan, S. Fano resonance based on metal-insulator-metal waveguide-coupled double rectan-gular cavities for plasmonic Sensors 16, 22–24 (2016). https://doi.org/10.3390/s16050642
  68. Chen, Z., Cui, L., Song, X., Yu, L. & Xiao, J. High sensitivity plasmonic sensing based on Fano interference in a rectangular ring waveguide. Opt. Commun. 340, 1–4 (2015). https://doi.org/10.1016/j.optcom.2014.11.081
  69. Tian, J., Wei, G., Yang, R. & Pei, W. Fano resonance and its application using a defective disk resonator coupled to an MDM plasmon waveguide with a nano-wall. Optik 208, 164136 (2020). https://doi.org/10.1016/j.ijleo.2019.164136
  70. Chou Chao, C.-T., Chou Chau, Y.-F & Chiang, H.-P. Multiple Fano resonance modes in an ultra-compact plasmonic waveguide-cavity system for sensing applications. Results 27, 104527 (2021). https://doi.org/10.1016/j.rinp.2021.104527
  71. Rakhshani, M. R. Optical refractive index sensor with two plasmonic double-square resonators for simultaneous sensing of human blood groups. Photonics 39, 100768 (2020). https://doi.org/10.1016/j.photonics.2020.100768
  72. Chen, Y., Xu, Y. & Cao, J. Fano resonance sensing characteristics of MIM waveguide coupled square convex ring resonator with metallic baffle. Results Phys. 14, 102420 (2019). https://doi.org/10.1016/j.rinp.2019.102420
  73. Ren, X., Ren, K. & Cai, Y. Tunable compact nanosensor based on Fano resonance in a plasmonic waveguide system. Appl. Opt. 56, H1–H9 (2017). https://doi.org/10.1364/AO.56.0000H1
  74. Tang, Y. et al. Refractive index sensor based on Fano resonances in metal-insulator-metal waveguides coupled with resonators. Sensors 17, 784 (2017). https://doi.org/10.3390/s17040784
  75. Yang, X., Hua, E., Su, H., Guo, J. & Yan, S. A nanostructure with defect based on Fano resonance for application on refractive-index and temperature sensing. Sensors 20, 4125 (2020). https://doi.org/10.3390/s20154125
  76. Chen, Y. et al. Sensing performance analysis on Fano resonance of metallic double-baffle contained MDM waveguide coupled ring resonator. Opt. Laser Technol. 101, 273–278 (2018). https://doi.org/10.1016/j.optlastec.2017.11.022
  77. Binfeng, Y., Ruohu, Z., Guohua, H. & Yiping, C. Ultra-sharp Fano resonances induced by coupling between plasmonic stub and circular cavity resonators. Plasmonics 11, 1157–1162 (2016). https://doi.org/10.1007/s11468-015-0154-5
  78. Zhang, Q., Huang, X.-G., Lin, X.-S., Tao, J. & Jin, X.-P. A subwavelength coupler-type MIM optical filter. Opt. Express 17, 7549–7554(2009). https://doi.org/10.1364/OE.17.007549
  79. Rakhshani, M. R. Fano resonances based on plasmonic square resonator with high figure of merits and its application in glucose concentrations sensing. Opt. Quantum 51, 287 (2019). https://doi.org/10.1007/s11082-019-2007-5
  80. Chen, F., Zhang, H., Sun, L., Li, J. & Yu, C. Temperature tunable Fano resonance based on ring resonator side coupled with a MIM waveguide. Opt. Laser Technol. 116, 293–299 (2019). https://doi.org/10.1016/j.optlastec.2019.03.044
  81. He, Y. et al. Convert from Fano resonance to electromagnetically induced transparency effect using anti-symmetric H-typed metamaterial resonator. Opt. Quantum Electron. 52, 391 (2020). https://doi.org/10.1007/s11082-020-02513-3
  82. Dionne, J. et al. A. Silicon-based plasmonics for on-chip photonics. IEEE J. Sel. Top. Quantum Electron. 16, 295–306 (2010). https://doi.org/10.1109/JSTQE.2009.2034983
  83. Zhan, S. et al. Tunable nanoplasmonic sensor based on the asymmetric degree of Fano resonance in MDM waveguide. Sci. Rep. 6, 22428 (2016). https://doi.org/10.1038/srep22428
  84. Guo, Z. et al. Plasmonic multichannel refractive index sensor based on subwavelength tangent-ring metal–insulator–metal waveguide. Sensors 18, 1348 (2018). https://doi.org/10.3390/s18051348
  85. Chen, Y., Chen, L., Wen, K., Hu, Y. & Lin, W. Multiple Fano resonances in a coupled plasmonic resonator system. J. Appl. Phys. 126, 083102 (2019). https://doi.org/10.1063/1.5105358
  86. Chen, Z., Song, X., Duan, G., Wang, L. & Yu, L. Multiple Fano resonances control in MIM side-coupled cavities systems. IEEE Photonics J. 7, 1–10 (2015). https://doi.org/10.1109/JPHOT.2015.2433012
  87. Zhang, X. et al. Refractive Index Sensor based on Fano resonances in plasmonic waveguide with dual side-coupled ring resonators. Photonic Sens. 8, 367– 374 (2018). https://doi.org/10.1007/s13320-018-0509-6
  88. Yang, X. et al. Fano resonance in a MIM waveguide with two triangle stubs coupled with a split-ring nanocavity for sensing application. Sensors 19, 4972 (2019). https://doi.org/10.3390/s19224972
  89. Wang, W.-D., Zheng, L. & Qi, J.-G. High Q-factor multiple Fano resonances for high-sensitivity sensing in all-dielectric nanocylinder dimer metamaterials. Appl. Express 12, 075002 (2019). https://doi.org/10.7567/1882-0786/ab206a
  90. Špačková, B., Wrobel, P., Bocková, M. & Homola, J. Optical biosensors based on plasmonic nanostructures: a review. Proc. IEEE 104, 2380–2408 (2016). https://doi.org/10.1109/JPROC.2016.2624340
  91. Li, S. et al. Fano resonances based on multimode and degenerate mode interference in plasmonic resonator system. Opt. Express 25, 3525–3533 (2017). https://doi.org/10.1364/OE.25.003525
  92. Butt, M. A., Kazanskiy, N. L. & Khonina, S. N. Nanodots decorated asymmetric metal-insulator-metal waveguide resonator structure based on Fano resonances for refractive index sensing Laser Phys. 30, (2020). https://doi.org/10.1088/1555-6611/ab9090
  93. Chen, Z., Cao, X. & Song, X. Side-coupled cavity-induced Fano resonance and its application in nanosensor. Plasmonics 11, 307– 313 (2016). https://doi.org/10.1007/s11468-015-0035-y
  94. Wang, Y., Li, S., Zhang, Y. & Yu, L. Independently formed multiple Fano resonances for ultra-high sensitivity plasmonic nanosensor. Plasmonics 13, 107– 113 (2018). https://doi.org/10.1007/s11468-016-0489-6
  95. Chen, J. et al. Fano resonance in a MIM waveguide with double symmetric rectangular stubs and its sensing characteristics. Opt. Commun. 482, 126563 (2021). https://doi.org/10.1016/j.optcom.2020.126563
  96. Chen, J. et al. Coupled-resonator-induced Fano resonances for plasmonic sensing with ultra-high figure of merits. Plasmonics 8, 1627–1631 (2013). https://doi.org/10.1007/s11468-013-9580-4
  97. Wen, K. et al. Fano resonance with ultra-high figure of merits based on plasmonic metal-insulator-metal waveguide. Plasmonics 10, 27–32 (2015). https://doi.org/10.1007/s11468-014-9772-6
  98. Yang, J. et al. Tunable multi-Fano resonances in MDM-based side-coupled resonator system and its application in nanosensor. Plasmonics 12, 1665–1672 (2017). https://doi.org/10.1007/s11468-016-0432-x
  99. Wen, K., Chen, L., Zhou, J., Lei, L. & Fang, Y. A Plasmonic chip-scale refractive index sensor design based on multiple Fano reso-nances. Sensors 18, 3181 (2018). https://doi.org/10.3390/s18103181
  100. Liu, Y. et al. Theoretical design of plasmonic refractive index sensor based on the fixed band detection. IEEE J. Sel. Top. Quantum Electron. 25, 1–6 (2019). https://doi.org/10.1109/JSTQE.2018.2827661
  101. Qiao, L., Zhang, G., Wang, Z., Fan, G. & Yan, Y. Study on the Fano resonance of coupling M-type cavity based on surface plasmon polaritons. Opt. Commun. 433, 144–149 (2019). https://doi.org/10.1016/j.optcom.2018.09.055
  102. Xiao, G. et al. High sensitivity plasmonic sensor based on Fano resonance with inverted u-shaped resonator. Sensors 21, 1–12 (2021). https://doi.org/10.3390/s21041164
  103. Li, C. et al. Multiple Fano resonances based on plasmonic resonator system with end-coupled cavities for high-performance nanosensor. IEEE Photonics J. 9, 1– 9 (2017). https://doi.org/10.1109/JPHOT.2017.2763781
  104. Shi, X. et al. Dual Fano resonance control and refractive index sensors based on a plasmonic waveguide-coupled resonator system. Opt. Commun. 427, 326–330 (2018). https://doi.org/10.1016/j.optcom.2018.06.042
  105. Chen, Z. et al. Sensing characteristics based on Fano resonance in rectangular ring waveguide. Opt. Commun. 356, 373–377 (2015). https://doi.org/10.1016/j.optcom.2015.08.020
  106. Wang, M., Zhang, M., Wang, Y., Zhao, R. & Yan, S. Fano resonance in an asymmetric MIM waveguide structure and its application in a refractive index nanosensor. Sensors 19, 791 (2019). https://doi.org/10.3390/s19040791
  107. Yu, S., Zhao, T., Yu, J. & Pan, D. Tuning multiple fano resonances for on-chip sensors in a plasmonic system. Sensors 19, 1559 (2019). https://doi.org/10.3390/s19071559
  108. Rahmatiyar, M., Danaie, M. & Afsahi, M. Employment of cascaded coupled resonators for resolution enhancement in plasmonic refractive index sensors. Opt. Quantum 52, 153 (2020). https://doi.org/10.1007/s11082-020-02266-z
  109. Li, Z. et al. Manipulation of multiple Fano resonances based on a novel chip-scale MDM structure. IEEE Access 8, 32914–32921 (2020). https://doi.org/10.1109/ACCESS.2020.2973417
  110. Fang, Y. et al. Multiple Fano resonances based on end-coupled semi-ring rectangular resonator. IEEE Photon. J. 11, 1–8 (2019). https://doi.org/1109/JPHOT.2019.2914483
  111. Wang, Q., Ouyang, Z., Sun, Y., Lin, M. & Liu, Q. Linearly tunable Fano resonance modes in a plasmonic nanostructure with a waveguide loaded with two rectangular cavities coupled by a circular Nanomaterials 9, 678 (2019). https://doi.org/10.3390/nano9050678
  112. Su, H. et al. Sensing features of the Fano resonance in an MIM waveguide coupled with an elliptical ring resonant cavity. Appl. Sci. 10, 5096 (2020). https://doi.org/10.3390/app10155096
  113. Wang, S., Zhao, T., Yu, S. & Ma, W. High-performance nano-sensing and slow-light applications based on tunable multiple Fano resonances and EIT-like effects in coupled plasmonic resonator IEEE Access 8, 40599–40611 (2020). https://doi.org/10.1109/ACCESS.2020.2974491
  114. Li, Z. et al. Control of multiple Fano resonances based on a subwavelength MIM coupled cavities system. IEEE Access 7, 59369–59375 (2019). https://doi.org/10.1109/ACCESS.2019.2914466
  115. El Haffar, R., Farkhsi, A. & Mahboub, O. Optical properties of MIM plasmonic waveguide with an elliptical cavity resonator. Appl. Phys. A 126, 486 (2020). https://doi.org/10.1007/s00339-020-03660-w
  116. Hassan, M. F., Hasan, M. M., Ahmed, M. I. & Sagor, R.H. Numerical investigation of a plasmonic refractive index sensor based on rectangular MIM topology. in 2020 International Seminar on Intelligent Technology and its Applications ISITIA 2020, 77–82 (IEEE, 2020). https://doi.org/10.1109/ISITIA49792.2020.9163755
  117. Wang, Y. et al. Design of sub wavelength-grating-coupled Fano resonance sensor in mid-infrared. Plasmonics 16, 463–469 (2021). https://doi.org/10.1007/s11468-020-01313-5
  118. Chen, Y., Chen, L., Wen, K., Hu, Y. & Lin, W. Double Fano resonances based on different mechanisms in a MIM plasmonic system. Photonics Nanostruct. 36, 100714 (2019). https://doi.org/10.1016/j.photonics.2019.100714
  119. Chen, Z., Chen, J., Yu, L. & Xiao, J. Sharp trapped resonances by exciting the anti-symmetric waveguide mode in a metal-insulator-metal resonator. Plasmonics 10, 131–137 (2015). https://doi.org/10.1007/s11468-014-9786-0
  120. Pang, S. et al. The sensing characteristics based on electro-magnetically-induced transparency-like response in double-sided stub and a nano-disk waveguide Mod. Phys. Lett. B 31, 1–9 (2017). https://doi.org/10.1142/S0217984917501019
  121. Zhang, Z. D. et al. Electromagnetically induced transparency and refractive index sensing for a plasmonic waveguide with a stub coupled ring resonator. Plasmonics 12, 1007–1013 (2017). https://doi.org/10.1007/s11468-016-0352-9
  122. Akhavan, A., Ghafoorifard, H., Abdolhosseini, S. & Habibiyan, H. Metal-insulator-metal waveguide-coupled asymmetric resonators for sensing and slow light IET Optoelectron. 12, 220–227 (2018). https://doi.org/10.1049/iet-opt.2018.0028
  123. Shi, H. et al. A nanosensor based on a metal-insulator-metal bus waveguide with a stub coupled with a racetrack ring resonator. Micromachines 12, 495 (2021). https://doi.org/10.3390/mi12050495
  124. Meng, Z.-M. & Qin, F. Realizing prominent Fano resonances in metal-insulator-metal plasmonic Bragg gratings side-coupled with plasmonic nanocavities. Plasmonics 13, 2329–2336 (2018). https://doi.org/10.1007/s11468-018-0756-9
  125. Tathfif, I., Rashid, K.S., Yaseer, A. A. & Sagor, R.H. Alternative material titanium nitride based refractive index sensor embedded with defects: An emerging solution in sensing Results Phys. 29, 104795 (2021). https://doi.org/10.1016/j.rinp.2021.104795
  126. Li, Q. et al. Active control of asymmetric Fano resonances with graphene–silicon-integrated terahertz metamaterials. Adv. Mater. Technol. 5, 1–7 (2020). https://doi.org/10.1002/admt.201900840
  127. Ge, J. et al. Tunable dual plasmon-induced transparency based on a monolayer graphene metamaterial and its terahertz sensing performance. Opt. Express 28, 31781–31795 (2020). https://doi.org/10.1364/OE.405348
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Authors and Affiliations

Rammani Adhikari
1 2
Diksha Chauhan
1
Genene T. Mola
3
Ram P. Dwivedi
1

  1. Faculty of Engineering and Technology, Shoolini University, Bajhol, (HP) 173229, India
  2. School of Engineering, Pokhara University, Pokhara Metropolitan City 30, Kaski, Nepal
  3. School of Chemistry and Physics, University of Kwazulu Natal, Scottsville, South Africa
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Abstract

The design and performance analysis of a 1310/1550-nm wavelength division demultiplexer with tapered geometry based on InP/InGaAsP multimode interference (MMI) coupler has been carried out. Wavelength response of demultiplexer of conventional MMI and tapered input and tapered output (tapered I/O) waveguides geometry of the MMI have been discussed. The demultiplexing function has been first performed by choosing a suitable refractive index of the guiding region and geometrical parameters such as the width and length of MMI structure have been achieved. Access width of tapered I/O waveguides have been adjusted to give a low insertion loss (IL) and high extinction ratio (ER) for the considered wavelengths of 1310 nm and 1550 nm. The total size of the demultiplexer has been significantly reduced over the existing MMI devices. Numerical simulations with finite difference beam propagation method are applied to design and optimize the operation of the proposed demultiplexer.

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Authors and Affiliations

D. Chack
V. Kumar
S.K. Raghuwanshi
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Abstract

The SIW antenna suffers from the narrow bandwidth for a single cavity and single resonant. Defected ground structure (DGS) with a dual cavity was the solution to solve narrow bandwidth by resulting in hybrid resonance. The hybrid resonance with 14.83% impedance bandwidth is proposed in this antenna design. The first resonance resulted from the combination of the TE101 modes from inner and outer HMSIW cavities while the second resonance resulted from the combination of the strong TE101 and the weak TE102 mode from the inner HMSIW cavity and the addition of the weak TE101 from the outer HMSIW cavity. The measurement antenna design has a broadband antenna with a 14.31% (5.71 – 6.59 GHz) impedance bandwidth by using substrate Rogers RO 5880.
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Authors and Affiliations

Dian Widi Astuti
1
Rivayanto
1
Muslim
1
Imelda Simanjuntak
1
Teguh Firmansyah
2
Dwi Astuti Cahyasiwi
3
Yus Natali
4

  1. Department of Electrical Engineering, Universitas Mercu Buana, Jakarta, Indonesia
  2. Department of Electrical Engineering, Universitas Sultan Ageng Tirtayasa, Serang, Indonesia
  3. Department of Electrical Engineering, Universitas Muhammadiyah Prof. Dr. HAMKA, Jakarta, Indonesia
  4. Telecommunication Program, Universitas Telkom, Jakarta, Indonesia
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Abstract

On-chip optical-interconnect technology emerges as an attractive approach due to its ultra-large bandwidth and ultra-low power consumption. Silicon-on-insulator (SOI) wire waveguides, on the other hand, have been identified to potentially replace copper wires for intra-chip communication. To take advantage of the wide bandwidth of SOI waveguides, wavelengthdivision multiplexing (WDM) has been implemented. However, WDM have inherent drawbacks. Mode-division multiplexing (MDM) is a viable alternative to WDM in MIMO photonic circuits on SOI as it requires only one carrier wavelength to operate. In this vein, mode converters are key components in on-chip MDM systems. The goal of this paper is to introduce a transverse electric mode converter. The suggested device can convert fundamental transverse electric modes to first-order transverse electric ones and vice versa. It is based on small material perturbation which introduces gradual coupling between different modes. This device is very simple and highly compact; the size of which is 3 μm2. Mathematical expressions for both the insertion loss and crosstalk are derived and optimized for best performance. In addition, three-dimensional finite-difference time-domain (3D-FDTD) simulations are performed in order to verify the mathematical model of the device. Our numerical results reveal that the proposed device has an insertion loss of 1.2 dB and a crosstalk of 10.1 dB. The device’s insertion loss can be decreased to 0.95 dB by adding tapers to its material perturbation.
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Authors and Affiliations

Mohamed H. Sharaf
1
Mohamed B. El-Mashade
1
Ahmed A. Emran
1

  1. Electrical Engineering Department, Faculty of Engineering, Al-Azhar University, Cairo, Egypt

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