journal article·2017-12

Perfect Terahertz Absorption with Graphene Surface Plasmons in the Modified Otto Configuration

Leyong Jiang, Jun Guo, Qingkai Wang, Xiaoyu Dai, Yuanjiang Xiang

Plasmonics· Volume 12· Issue 6
Publisher page

Abstract

Perfect terahertz (THz) absorption in the modified Otto configuration with the insertion of monolayer graphene sheet has been numerically demonstrated. This perfect absorption originates from the enhancement of the electrical field owing to the excitation of the transverse magnetic (TM) polarized surface plasmons at the interface of two dielectrics with monolayer graphene. It is found that the absorption peak occurs at the specific incident angles, which can be employed for realizing the angular absorbers. We further demonstrate that the angle of the peak absorption and the corresponding wavelength can be manipulated by changing the Fermi energy of monolayer graphene sheet via electrostatic biasing. Moreover, the behaviors of the perfect absorption are strongly dependent on the dielectric constants and thicknesses of the surrounding dielectrics.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Metamaterials and Metasurfaces Applications · Plasmonic and Surface Plasmon Research · Photonic Crystals and Applications

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

References (33)

Show source-provided references
1. Chen HT (2012) Interference theory of metamaterial perfect absorbers. Opt Express 20(7):7165–717210.1364/OE.20.007165 ↗
2. Tonouchi M (2007) Cutting-edge terahertz technology. Nat Photonics 1(2):97–10510.1038/nphoton.2007.3 ↗
3. Thongrattanasiri S, Koppens FHL, García de Abajo FJ (2012) Complete optical absorption in periodically patterned graphene. Phys Rev Lett 108(4):04740110.1103/PhysRevLett.108.047401 ↗
4. Liu N, Mesch M, Weiss T, Hentschel M, Giessen H (2010) Infrared perfect absorber and its application asplasmonic sensor. Nano Lett 10(7):2342–234810.1021/nl9041033 ↗
5. Landy NI, Sajuyigbe S, Mock JJ, Smith DR, Padilla WJ (2008) Perfect metamaterial absorber. Phys Rev Lett 100(20):20740210.1103/PhysRevLett.100.207402 ↗
6. Tao H, Landy NI, Bingham CM, Zhang X, Averitt RD, Padilla WJ (2008) A metamaterial absorber for the terahertz regime: design, fabrication and characterization. Opt Express 16(10):7181–718810.1364/OE.16.007181 ↗
7. Halterman K, Elson JM (2014) Near-perfect absorption in epsilon-near-zero structures with hyperbolic dispersion. Opt Express 22(6):7337–734810.1364/OE.22.007337 ↗
8. Kakimi R, Fujita M, Nagai M, Ashida M, Nagatsuma T (2014) Capture of a terahertz wave in a photonic-crystal slab. Nat Photonics 8(8):657–66310.1038/nphoton.2014.150 ↗
9. Ye YQ, Jin Y, He S (2010) Omnidirectional, polarization-insensitive and broadband thin absorber in the terahertz regime. J Opt Soc Am B 27(3):498–50410.1364/JOSAB.27.000498 ↗
10. Holloway CL, Kuester EF, Gordon JA, O'Hara J, Booth J, Smith DR (2012) An overview of the theory and applications of metasurfaces: the two-dimensional equivalents of metamaterials. IEEE Antennas Propag 54(2):10–3510.1109/MAP.2012.6230714 ↗
11. Novoselov KS, Geim AK, Morozov SV, Jiang D, Zhang Y, Dubonos SV, Grigorieva IV, Firsov AA (2004) Electric field effect in atomically thin carbon films. Science 306(5696):666–66910.1126/science.1102896 ↗
12. Neto AHC, Guinea F, Peres NMR, Novoselov KS, Geim AK (2009) The electronic properties of graphene. Rev Mod Phys 81(1):109–16210.1103/RevModPhys.81.109 ↗
13. Koppens FHL, Chang DE, García de Abajo FJ (2011) Graphene plasmonics: a platform for strong light matter interactions. Nano Lett 11(8):3370–337710.1021/nl201771h ↗
14. Mikhailov SA, Ziegler K (2008) Nonlinear electromagnetic response of graphene: frequency multiplication and the self-consistent-field effects. J Phys Condens Matter 20(38):38420410.1088/0953-8984/20/38/384204 ↗
15. Kim JT, Yu YJ, Choi H, Choi CG (2014) Graphene-based plasmonic photodetector for photonic integrated circuits. Opt Express 22(1):803–80810.1364/OE.22.000803 ↗
16. Huang PL, Lin SC, Yeh CY, Kuo HH, Huang SH, Lin GR, Li LJ, Su CY, Cheng WH (2012) Stable mode-locked fiber laser based on CVD fabricated graphene saturable absorber. Opt Express 20(3):2460–246510.1364/OE.20.002460 ↗
17. Liu M, Yin X, Avila EU, Geng B, Zentgraf T, Ju L, Wang F, Zhang X (2011) A graphene-based broadband optical modulator. Nature 474(7349):64–6710.1038/nature10067 ↗
18. Bludov YV, Vasilevskiy MI, Peres NMR (2012) Tunable graphene-based polarizer. J Appl Phys 112(8):08432010.1063/1.4759319 ↗
19. Bludov YV, Vasilevskiy MI, Peres NMR (2010) Mechanism for graphene-based optoelectronic switches by tuning surface plasmon-polaritons in monolayer graphene. Europhys Lett 92(6):6800110.1209/0295-5075/92/68001 ↗
20. Han TH, Lee Y, Choi MR, Woo SH, Bae SH, Hong BH, Ahn JH, Lee TW (2010) Extremely efficient flexible organic light-emitting diodes with modified graphene anode. Nat Photonics 6(2):105–11010.1038/nphoton.2011.318 ↗
21. Xiang Y, Dai X, Guo J, Wen S, Tang D (2014) Tunable optical bistability at the graphene-covered nonlinear interface. Appl Phys Lett 104(5):05110810.1063/1.4863927 ↗
22. Deng XH, Liu JT, Yuan J, Wang TB, Liu NH (2014) Tunable THz absorption in graphene-based heterostructures. Opt Express 22(24):30177–3018310.1364/OE.22.030177 ↗
23. Woo JM, Kim MS, Kim HW, Jang JH (2014) Graphene based salisbury screen for terahertz absorber. Appl Phys Lett 104(8):08110610.1063/1.4866665 ↗
24. Xu B, Gu C, Li Z, Niu Z (2013) A novel structure for tunable terahertz absorber based on graphene. Opt Express 21(20):23803–2381110.1364/OE.21.023803 ↗
25. Mikhailov SA, Ziegler K (2007) New electromagnetic mode in graphene. Phys Rev Lett 99(1):01680310.1103/PhysRevLett.99.016803 ↗
26. Grigorenko AN, Polini M, Novoselov KS (2012) Graphene plasmonics. Nat Photonics 6(11):749–75810.1038/nphoton.2012.262 ↗
27. Lin IT, Liu JM (2014) Enhanced graphene plasmon waveguiding in a layered graphene–metal structure. Appl Phys Lett 105(1):01160410.1063/1.4889915 ↗
28. Dai X, Jiang L, Xiang Y (2015) Tunable THz angular/frequency filters in the modified Kretschmann–Raether configuration with the insertion of single layer graphene. IEEE Photonics J 7(2):5500808
29. Zhan T, Shi X, Dai Y, Liu X, Zi J (2013) Transfer matrix method for optics in graphene layers. J Phys Condens Matter 25(21):21530110.1088/0953-8984/25/21/215301 ↗
30. Chen CF, Park CH, Boudouris CH, Horng J, Geng B, Girit C, Wang F (2011) Controlling inelastic lightscattering quantum pathways in graphene. Nature 471(7340):617–62010.1038/nature09866 ↗
31. Efetov DK, Kim P (2010) Controlling electron-phonon interactions in graphene at ultrahigh carrier densities. Phys Rev Lett 105(25):25680510.1103/PhysRevLett.105.256805 ↗
32. García de Abajo FJ (2010) Graphene plasmonics: challenges and opportunities. ACS Photonics 1(3):135–15210.1021/ph400147y ↗
33. Foley JJ IV, Harutyunyan H, Rosenmann D, Divan R, Wiederrecht GP, Gray SK (2015) When are surface plasmon polaritons excited in the Kretschmann-Raether configuration? Sci Rep 5:992910.1038/srep09929 ↗