journal article·2024-04

Slow Light Realization Based on Plasmon-Induced Transparency in Γ-Shaped Rectangular Resonator Structures

Samira Taghizadehasl Foroughi, Reza Yadipour, Saeed Golmohammadi, Tofiq Nurmohammadi

Plasmonics· Volume 19· Issue 2
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Abstract

In this study, Γ-shaped rectangular resonators, which are created in a metal insulator metal (MIM) structure, have been studied analytically and numerically. The metal is silver and rectangular resonators are filled by Si and the peak of transparency profile is tuned in the communication band with proper geometrical parameters. By employing 2-D finite difference time domain method (FDTD), simulations show a plasmonic induced transparency (PIT) window in the transmission diagram. The PIT is created by instructive and destructive interference between bright and dark resonator modes. The presented structure demonstrates tunable transparency window by variation of symmetry parameter, s. The maximum group velocity is obtained 0.1 ps in communication band corresponded to 30 μm traveling of light in the vacuum which is comparable to previous articles. The proposed structure may have potential applications in optical memory and delay blocks in designing integrated optical circuits.
Source: expertdata · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Plasmonic and Surface Plasmon Research · Photonic and Optical Devices · Photonic Crystals and Applications

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (53)

Show source-provided references
1. Atwater HA (2007) The promise of plasmonics. Sci Am 296(4):56–6310.1038/scientificamerican0407-56 ↗
2. Barnes WL, Dereux A, Ebbesen TW (2003) Surface plasmon subwavelength optics nature. 424(6950):824–830
3. Raether H (2006) Surface plasmons on smooth surfaces. Surface plasmons on smooth and rough surfaces and on gratings. 19:4–39
4. Kurokawa Y, Miyazaki HT (2007) Metal-insulator-metal plasmon nanocavities: analysis of optical properties. Phys Rev B 75(3):03541110.1103/PhysRevB.75.035411 ↗
5. Kamada S, Okamoto T, El-Zohary SE, Haraguchi M (2016) Design optimization and fabrication of Mach-Zehnder interferometer based on MIM plasmonic waveguides. Opt Express 24(15):16224–1623110.1364/OE.24.016224 ↗
6. Nurmohammadi T, Abbasian K, Yadipour R (2018) Ultra-fast all-optical plasmonic switching in near infra-red spectrum using a Kerr nonlinear ring resonator. Opt Commun 1(410):142–14710.1016/j.optcom.2017.09.082 ↗
7. Pu M, Yao N, Hu C, Xin X, Zhao Z, Wang C, Luo X (2010) Directional coupler and nonlinear Mach-Zehnder interferometer based on metal-insulator-metal plasmonic waveguide. Opt Express 18(20):21030–2103710.1364/OE.18.021030 ↗
8. Nurmohammadi T, Abbasian K, Yadipour R (2017) A proposal for a demultiplexer based on plasmonic metal–insulator–metal waveguide-coupled ring resonator operating in near-infrared spectrum. Optik 1(142):550–55610.1016/j.ijleo.2017.05.109 ↗
9. Kou Y, Chen X (2011) Multimode interference demultiplexers and splitters in metal-insulator-metal waveguides. Opt Express 19(7):6042–604710.1364/OE.19.006042 ↗
10. Nurmohammadi T, Abbasian K, Yadipour R (2018) Numerical study of dumbbell-shaped gold nanoparticles using in plasmonic waveguides in near infra-red spectrums. Opt Quant Electron 50:1–310.1007/s11082-018-1457-5 ↗
11. Babicheva VE, Lavrinenko AV (2013) A plasmonic modulator based on metal-insulator-metal waveguide with barium titanate core. Photonics Lett Poland 5(2):57–5910.4302/plp.2013.2.08 ↗
12. Khatooni HS, Abbasian K, Nurmohammadi T (2020) A tunable band-stop plasmonic waveguide filter and switch designing with triangular resonator based on Kerr non-linearity. Optik 1(224):16570810.1016/j.ijleo.2020.165708 ↗
13. Chen L, Lu P, Tian M, Liu D, Zhang J (2013) A subwavelength MIM waveguide filter with single-cavity and multi-cavity structures. Optik-International Journal for Light and Electron Optics 124(18):3701–370410.1016/j.ijleo.2012.11.025 ↗
14. Muñoz P, Yong YS, Dijkstra M, Segerink FB, García-Blanco SM (2019) Double metal layer lift-off process for the robust fabrication of plasmonic nano-antenna arrays on dielectric substrates using e-beam lithography. Opt Mater Express 9(5):2046–205610.1364/OME.9.002046 ↗
15. Zhu B, Chen M, Zhu Q, Zhou G, Abdelazim NM, Zhou W, Kershaw SV, Rogach AL, Zhao N, Tsang HK (2019) Integrated plasmonic infrared photodetector based on colloidal HgTe quantum dots. Adv Mater Technol 4(10):190035410.1002/admt.201900354 ↗
16. Fu Y, Hu X, Lu C, Yue S, Yang H, Gong Q (2012) All-optical logic gates based on nanoscale plasmonic slot waveguides. Nano Lett 12(11):5784–579010.1021/nl303095s ↗
17. Peters RF, Gutierrez-Rivera L, Dew SK, Stepanova M (2015) Surface enhanced Raman spectroscopy detection of biomolecules using EBL fabricated nanostructured substrates. JoVE (Journal of Visualized Experiments) 97:e52712
18. Tuniz A (2021) Nanoscale nonlinear plasmonics in photonic waveguides and circuits. La Rivista del Nuovo Cimento 44(4):193–24910.1007/s40766-021-00018-7 ↗
19. Nielsen MP, Shi X, Dichtl P, Maier SA, Oulton RF (2017) Giant nonlinear response at a plasmonic nanofocus drives efficient four-wave mixing. Science 358(6367):1179–118110.1126/science.aao1467 ↗
20. Gersen H, Karle TJ, Engelen RJ, Bogaerts W, Korterik JP, Van Hulst NF, Krauss TF, Kuipers L (2005) Real-space observation of ultraslow light in photonic crystal waveguides. Phys Rev Lett 94(7):07390310.1103/PhysRevLett.94.073903 ↗
21. Zhang Y, Hayasaka K, Kasai K (2005) Conditional transfer of quantum correlation in the intensity of twin beams. Phys Rev A 71(6):06234110.1103/PhysRevA.71.062341 ↗
22. Harris SE, Hau LV (1999) Nonlinear optics at low light levels. Phys Rev Lett 82(23):461110.1103/PhysRevLett.82.4611 ↗
23. Piao X, Yu S, Park N (2012) Control of Fano asymmetry in plasmon induced transparency and its application to plasmonic waveguide modulator. Opt Express 20(17):18994–1899910.1364/OE.20.018994 ↗
24. Wang J, Niu Y, Liu D, Hu ZD, Sang T, Gao S (2018) Tunable plasmon-induced transparency effect in MIM side-coupled isosceles trapezoid cavities system. Plasmonics 13:609–61610.1007/s11468-017-0551-z ↗
25. Han X, Wang T, Li X, Liu B, He Y, Tang J (2015) Dynamically tunable slow light based on plasmon induced transparency in disk resonators coupled MDM waveguide system. J Phys D Appl Phys 48(23):23510210.1088/0022-3727/48/23/235102 ↗
26. Wang G, Zhang W, Gong Y, Liang J (2014) Tunable slow light based on plasmon-induced transparency in dual-stub-coupled waveguide. IEEE Photonics Technol Lett 27(1):89–9210.1109/LPT.2014.2362293 ↗
27. Zhang Z, Yang J, He X, Han Y, Zhang J, Huang J, Chen D, Xu S (2018) Active enhancement of slow light based on plasmon-induced transparency with gain materials. Materials 11(6):94110.3390/ma11060941 ↗
28. Tian J, Li J (2020) Investigation on plasmon induced transparency and its application in an MIM type compound plasmonic waveguide. Progress In Electromagnetics Research C 98:199–21210.2528/PIERC19102001 ↗
29. Chen CY, Un IW, Tai NH, Yen TJ (2009) Asymmetric coupling between subradiant and superradiant plasmonic resonances and its enhanced sensing performance. Opt Express 17(17):15372–1538010.1364/OE.17.015372 ↗
30. Chen Z, Dai L, Jiang C (2011) Polarization-independent plasmon-induced transparency for plasmonic sensing. J Phys D Appl Phys 44(32):32510610.1088/0022-3727/44/32/325106 ↗
31. Zhan S, Li H, Cao G, He Z, Li B, Xu H (2014) Theoretical analysis of plasmon-induced transparency in ring-resonators coupled channel drop filter systems. Plasmonics 9:1431–143710.1007/s11468-014-9760-x ↗
32. Xiao S, Wang T, Liu T, Yan X, Li Z, Xu C (2018) Active modulation of electromagnetically induced transparency analogue in terahertz hybrid metal-graphene metamaterials. Carbon 1(126):271–27810.1016/j.carbon.2017.10.035 ↗
33. Yan X, Wang T, Xiao S, Liu T, Hou H, Cheng L, Jiang X (2017) Dynamically controllable plasmon induced transparency based on hybrid metal-graphene metamaterials. Sci Rep 7(1):1391710.1038/s41598-017-14328-6 ↗
34. Nurmohammadi T, Abbasian K, Mashayekhi MZ (2022) Graphene-based tunable plasmon-induced transparency utilizing circular and two rectangular gold rings in the near-infrared spectrum. Mater Sci Semicond Process 15(144):10660110.1016/j.mssp.2022.106601 ↗
35. Han Z, Bozhevolnyi SI (2011) Plasmon-induced transparency with detuned ultracompact Fabry-Perot resonators in integrated plasmonic devices. Opt Express 19(4):3251–325710.1364/OE.19.003251 ↗
36. Zhan S, Li H, Cao G, He Z, Li B, Yang H (2014) Slow light based on plasmon-induced transparency in dual-ring resonator-coupled MDM waveguide system. J Phys D Appl Phys 47(20):20510110.1088/0022-3727/47/20/205101 ↗
37. Lu H, Liu X, Mao D (2012) Plasmonic analog of electromagnetically induced transparency in multi-nanoresonator-coupled waveguide systems. Phys Rev A 85(5):05380310.1103/PhysRevA.85.053803 ↗
38. Kekatpure RD, Barnard ES, Cai W, Brongersma ML (2010) Phase-coupled plasmon-induced transparency. Phys Rev Lett 104(24):24390210.1103/PhysRevLett.104.243902 ↗
39. Wang T, Zhang Y, Hong Z, Han Z (2014) Analogue of electromagnetically induced transparency in integrated plasmonics with radiative and subradiant resonators. Opt Express 22(18):21529–2153410.1364/OE.22.021529 ↗
40. Zhang Z, Zhang L, Li H, Chen H (2014) Plasmon induced transparency in a surface plasmon polariton waveguide with a comb line slot and rectangle cavity. Appl Phys Lett 104(23)10.1063/1.4883647 ↗
41. Guo Y, Yan L, Pan W, Luo B, Wen K, Guo Z, Luo X (2012) Electromagnetically induced transparency (EIT)-like transmission in side-coupled complementary split-ring resonators. Opt Express 20(22):24348–2435510.1364/OE.20.024348 ↗
42. Pav M, Pooretemad S, Granpayeh N (2023) Ultra-fast all-optical plasmonic dual-band nonlinear off–on and two-port switches. Plasmonics 4:1–1
43. Yang HU, D’Archangel J, Sundheimer ML, Tucker E, Boreman GD, Raschke MB (2015) Optical dielectric function of silver. Phys Rev B 91(23):23513710.1103/PhysRevB.91.235137 ↗
44. Johnson PB, Christy RW (1972) Optical constants of the noble metals. Phys Rev B 6(12):437010.1103/PhysRevB.6.4370 ↗
45. Maier SA (2007) Plasmonics: fundamentals and applications. New York: springer10.1007/0-387-37825-1 ↗
46. Chen ZQ, Qi JW, Chen J, Li YD, Hao ZQ, Lu WQ, Xu JJ, Sun Q (2013) Fano resonance based on multimode interference in symmetric plasmonic structures and its applications in plasmonic nanosensors. Chin Phys Lett 30(5):05730110.1088/0256-307X/30/5/057301 ↗
47. Zhao X, Zhang Z, Yan S (2017) Tunable Fano resonance in asymmetric MIM waveguide structure. Sensors 17(7):149410.3390/s17071494 ↗
48. Hu F, Yi H, Zhou Z (2011) Band-pass plasmonic slot filter with band selection and spectrally splitting capabilities. Opt Express 19(6):4848–485510.1364/OE.19.004848 ↗
49. Xiao B, Tong S, Fyffe A, Shi Z (2020) Tunable electromagnetically induced transparency based on graphene metamaterials. Opt Express 28(3):4048–405710.1364/OE.382485 ↗
50. Linder J, Halterman K (2016) Dynamical tuning between nearly perfect reflection, absorption, and transmission of light via graphene/dielectric structures. Sci Rep 6(1):110.1038/srep38141 ↗
51. Xie Y, Chai J, Ye Y, Song T, Liu B, Zhang L, Zhu Y, Liu Y (2021) A tunable slow light device with multiple channels based on plasmon-induced transparency. Plasmonics 16:1809–181610.1007/s11468-020-01367-5 ↗
52. Wen K, Hu Y, Chen L, Zhou J, He M, Lei L, Meng Z (2016) Plasmonic-induced absorption and transparency based on a compact ring-groove joint MIM waveguide structure. IEEE Photonics J 8(5):1–8
53. Fan H, Tian J, Yang R (2023) Study of Fano resonance and its application in MIM waveguide using a k-shaped resonator. Opt Quant Electron 55(1):7510.1007/s11082-022-04297-0 ↗