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Plasmonics

, Volume 14, Issue 2, pp 511–521 | Cite as

Design and Simulation of a High-Selective Plasmon-Induced Reflectance in Coupled Dielectric-Metal-Dielectric Nano-structure for Senor Devices and Slow Light Propagation

  • Abbas Hamooleh Alipour
  • Ali MirEmail author
Article
  • 155 Downloads

Abstract

A new framework of high-selective plasmonic-induced reflectance (PIR) in a plasmonic-induced transparency (PIT) system is presented by using planar dielectric-metal-dielectric (DMD) metamaterial nano-structure. We used glass as substrate, the first dielectric, gold as metal thin film, and prism as the second dielectric. The proposed plasmonic nano-structure has been investigated based on finite difference time domain (FDTD) method. Results show that by coupling incident light with dark and bright plasmonic modes, without losing the metamaterial structure symmetry, the transparent window is created at 1550 nm and can be tuned. The transmittance (T), reflectance (R), and absorbance (A) coefficients of the presented nano-structure can be considerably varied by changing the thickness of thin films and dimension of the strips. The reflectance coefficients of dip1 (200 THz) and dip2 (265.5 THz) are almost near zero, and the transmittance coefficient of PIR (227.1 THz) is 0.93. Also, the maximum sensitivity and figure of merit are 664 and 3.77 for reflectance dip2, respectively. Similarly, the maximum quality factor (Q) is 10.74 for reflectance dip1. The presented plasmonic metamaterial nano-structure with mentioned unique features is a good candidate for several applications such as multi-channel plasmonic filters, bio and refractive index sensors, optical antenna, and slow-light devices for using in optical nano-electronic circuits and systems.

Keywords

Plasmonic Sensor device Slow-light device Refractive index Sensitivity 

References

  1. 1.
    Maier SA (2007) Plasmonics: fundamentals and applications. Springer, New YorkCrossRefGoogle Scholar
  2. 2.
    Szunerits S, Boukherroub R (2015) Introduction to plasmonics advances and applications. CRC Press, Taylor & Francis Group, DanverCrossRefGoogle Scholar
  3. 3.
    Shvets G, Tsukerman I (2012) Analysis and Applications. In: Plasmonics and plasmonic metamaterials. World Scientific, DanverGoogle Scholar
  4. 4.
    Zhang S, Genov DA, Wang Y, Liu M, and Zhang X (2008) “Plasmon-induced transparency in metamaterials,” Phys Rev Lett, 101:(4)Google Scholar
  5. 5.
    Vafapour Z, Forouzeshfard MR (2017) Disappearance of plasmonically induced reflectance by breaking symmetry in metamaterials. Plasmonics 12(5):1331–1342CrossRefGoogle Scholar
  6. 6.
    Vafapour Z, Zakery A (2016) New approach of plasmonically induced reflectance in a planar metamaterial for plasmonic sensing applications. Plasmonics 11(2):609–618CrossRefGoogle Scholar
  7. 7.
    Liu N, Weiss T, Mesch M, Langguth L, Eigenthaler U, Hirscher M, Sonnichsen C, Giessen H (2016) Planar metamaterial analogue of electromagnetically induced transparency for plasmonic sensing. Nano Lett 10(4):1103–1107CrossRefGoogle Scholar
  8. 8.
    Keshavarz A, Zakery A (2017) A novel terahertz semiconductor metamaterial for slow light device and dual-band modulator applications. Plasmonics:1–8Google Scholar
  9. 9.
    Vafapour Z, Alaei H (2016) Subwavelength micro-antenna for achieving slow light at microwave wavelengths via electromagnetically induced transparency in 2D metamaterials. Plasmonics 12(5):1343–1352CrossRefGoogle Scholar
  10. 10.
    Vafapour Z, Alaei H (2017) Achieving a high Q-factor and tunable slow-light via classical electromagnetically induced transparency (Cl-EIT) in metamaterials. Plasmonics 12(2):479–488CrossRefGoogle Scholar
  11. 11.
    Vafapour Z, Zakery A (2015) New regime of plasmonically induced transparency. Plasmonics 10(6):1809–1815CrossRefGoogle Scholar
  12. 12.
    Ding J, Arigong B, Ren H, Zhou M, Shao J, Lu M, Chai Y, Lin Y, Zhang H (2014) Tuneable complementary metamaterial structures based on graphene for single and multiple transparency windows. Sci Rep:1–7Google Scholar
  13. 13.
    Shi S, Wei Z, Lu Z, Zhang X, Li X, Liu H, Liang R (2015) Enhanced plasmonic band-pass filter with symmetric dual side-coupled nanodisk resonators. J Appl Phys 118(14)Google Scholar
  14. 14.
    Gao X, Zhou L, Cui TJ (2015) Odd-mode surface plasmon polaritons supported by complementary plasmonic metamaterial. Sci Rep:1–5Google Scholar
  15. 15.
    Mahani FF, Mokhtari A, Mehran M (2017) Dual mode operation, highly selective nanohole array-based plasmonic colour filters. Nanotechnology:1–9Google Scholar
  16. 16.
    Keleshtery MH, Mir A, Kaatuzian H (2017) Investigating the characteristics of a double circular ring resonators slow light device based on the plasmonics-induced transparency coupled with metal-dielectric-metal waveguide system. Plasmonics:1–12Google Scholar
  17. 17.
    Xia F, Sekaric L, Vlasov Y (2006) Ultracompact optical buffers on a silicon chip. Nat Photonics:65–71Google Scholar
  18. 18.
    Chen N, Pitchappa P, Ho CP, Hasan D, Kropelnicki P, Alioto M, Lee C (2016) Polarization controllable multispectral symmetry-breaking absorber in mid-infrared. J Appl Phys 120(6):063105–063108CrossRefGoogle Scholar
  19. 19.
    Chen X and Fan W (2017) “Ultrasensitive terahertz metamaterial sensor based on spoof surface plasmon,” Scientific Reports, pp. 1–8Google Scholar
  20. 20.
    Farmani A, Zarifkar A, Sheikhi MH, Miri M (Dec. 2017) Design of a tunable graphene plasmonic-on-white graphene switch at infrared range. Superlattice Microst 112:404–414CrossRefGoogle Scholar
  21. 21.
    Xu M, Li F, Wang T, Wu J, Lu L, Zhou L, Su Y (2013) Design of an electro-optic modulator based on a silicon-plasmonic hybrid phase shifter. J Of Lightwave Technol 31(8):1170–1177CrossRefGoogle Scholar
  22. 22.
    Hatta AM, Kamli AA, Al-Hagan OA, Moiseev SA (2015) Slow light with electromagnetically induced transparency in optical fibre. J Phys B: Atomic Mol Opt Phys 48(7):15502Google Scholar
  23. 23.
    Yang J, Yang S, Song X, Wu F and Yu L (2017) “Active control of slow light in a gain-assisted plasmon-induced transparency structure,” IEEE Photonics J, 9Google Scholar
  24. 24.
    Neveu P, Maynard MA, Bouchez R, Lugani J, Ghosh R, Bretenaker F, Goldfarb F, and Brion E (2017) “Coherent population oscillation-based light storage,” Phys Rev Lett, 118Google Scholar
  25. 25.
    Wang X, Zhou P, Wang X, Xiao H, and Liu Z (2015) “Tunable slow light via stimulated Brillouin scattering at 2 μm based on Tm-doped fiber amplifiers,” Opt Lett , 40(11)
  26. 26.
    Liang JQ, Katsuragawa M, Kien FL, and Hakuta K (2002) “Slow light produced by stimulated Raman scattering in solid hydrogen,” Phys Rev A, 65Google Scholar
  27. 27.
    Ye Y, Xie Y, Liu Y, Wang S, Zhang J, Liu Y (2017) Design of a compact logic device based on plasmon-induced transparency. IEEE Photonics Technology Let 29(8):647–650CrossRefGoogle Scholar
  28. 28.
    Prabhathan1 P, Murukeshan VM (2016) Surface plasmon polariton-coupled waveguide back reflector in thin-film silicon solar cell. Plasmonics 11(1):253–260Google Scholar
  29. 29.
    Ji L, Sun X, He G, Liu Y, Wang X, Yi Y, Chen C, Wang F, Zhang D (2017) Surface plasmon resonance refractive index sensor based on ultraviolet bleached polymer waveguide. Sensors Actuators B Chem 244:373–379CrossRefGoogle Scholar
  30. 30.
    H-J Li, X. Zhai, R. Wujiaihemaiti, L-L W. and X-F. Li, “Tunable optical filters and multichannel switches based on MIM plasmonic nanodisk resonators inset a silver bar” IOP. Physica Scripta, 90:015604(6pp), 2014Google Scholar
  31. 31.
    Keleshtery MH, Kaatuzian H, Mir A, Zandi A (2017) Method proposing a slow light ring resonatorstructure coupled with a metal–dielectric– metal waveguide system based on plasmonic induced transparency. Applied Optics 56(15):4496–4504CrossRefGoogle Scholar
  32. 32.
    Liang Y, Zhang S, Cao X, Lu Y, Xu T (Jun. 2017) Free-standing plasmonic metal-dielectric-metal bandpass filter with high transmission efficiency. Sci Rep:1–8Google Scholar
  33. 33.
    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 48:235102(10ppCrossRefGoogle Scholar
  34. 34.
    Vafapour Z (Mar. 2017) Near infrared biosensor based on classical electromagnetically induced reflectance (Cl-EIR) in a planar complementary metamaterial. Opt Commun 387:1–11CrossRefGoogle Scholar
  35. 35.
    Wei Z, Li X, Zhong N, Tan X, Zhang X, Liu H, Meng H, Liang R (2017) Analogue electromagnetically induced transparency based on low-loss metamaterial and its application in nanosensor and slow-light device. Plasmonics 12(3):641–647CrossRefGoogle Scholar
  36. 36.
    Wu J, Jin B, Wan J, Liang L, Zhang Y, Jia T, Cao C, Kang L, Xu W, Chen J, Wu P (2011) Superconducting terahertz metamaterials mimicking electromagnetically induced transparency. Appl Phys Lett 99(16):161113(3)Google Scholar

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© Springer Science+Business Media, LLC, part of Springer Nature 2018

Authors and Affiliations

  1. 1.Department of Electronics, Faculty of EngineeringLorestan UniversityKhorram-AbadIran

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