High Absorption and Second-Harmonic Generation in Split Ring Resonator Multilayer Nanostructure
Second-harmonic generation in split ring resonator multilayer nanostructure is studied with the finite-difference time-domain (FDTD) method. The fundamental frequency wave and the second-harmonic generation at the resonant absorption wavelength are highly localized in the dielectric layer, and the a...
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| Published in | Journal of nanomaterials Vol. 2014; no. 2014; pp. 1 - 7 |
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| Main Authors | , , , , , , , |
| Format | Journal Article |
| Language | English |
| Published |
Cairo, Egypt
Hindawi Publishing Corporation
01.01.2014
Hindawi Limited |
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| Online Access | Get full text |
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| Abstract | Second-harmonic generation in split ring resonator multilayer nanostructure is studied with the finite-difference time-domain (FDTD) method. The fundamental frequency wave and the second-harmonic generation at the resonant absorption wavelength are highly localized in the dielectric layer, and the absorption peak is sensitive to dielectric constant of the dielectric layer. Under the excitation of the plasmon resonances mode, the strong local field induces an expected increase of the second-harmonic generation with conversion efficiencies 10−6-10−7. The distributions of fundamental frequency electric field and second-harmonic electric field inside the central dielectric layer region are also shown. |
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| AbstractList | Second-harmonic generation in split ring resonator multilayer nanostructure is studied with the finite-difference time-domain (FDTD) method. The fundamental frequency wave and the second-harmonic generation at the resonant absorption wavelength are highly localized in the dielectric layer, and the absorption peak is sensitive to dielectric constant of the dielectric layer. Under the excitation of the plasmon resonances mode, the strong local field induces an expected increase of the second-harmonic generation with conversion efficiencies 10 super(-6) -10 super(-7) . The distributions of fundamental frequency electric field and second-harmonic electric field inside the central dielectric layer region are also shown. Second‐harmonic generation in split ring resonator multilayer nanostructure is studied with the finite‐difference time‐domain (FDTD) method. The fundamental frequency wave and the second‐harmonic generation at the resonant absorption wavelength are highly localized in the dielectric layer, and the absorption peak is sensitive to dielectric constant of the dielectric layer. Under the excitation of the plasmon resonances mode, the strong local field induces an expected increase of the second‐harmonic generation with conversion efficiencies 10 −6 ‐10 −7 . The distributions of fundamental frequency electric field and second‐harmonic electric field inside the central dielectric layer region are also shown. Second-harmonic generation in split ring resonator multilayer nanostructure is studied with the finite-difference time-domain (FDTD) method. The fundamental frequency wave and the second-harmonic generation at the resonant absorption wavelength are highly localized in the dielectric layer, and the absorption peak is sensitive to dielectric constant of the dielectric layer. Under the excitation of the plasmon resonances mode, the strong local field induces an expected increase of the second-harmonic generation with conversion efficiencies 10−6-10−7. The distributions of fundamental frequency electric field and second-harmonic electric field inside the central dielectric layer region are also shown. Second-harmonic generation in split ring resonator multilayer nanostructure is studied with the finite-difference time-domain (FDTD) method. The fundamental frequency wave and the second-harmonic generation at the resonant absorption wavelength are highly localized in the dielectric layer, and the absorption peak is sensitive to dielectric constant of the dielectric layer. Under the excitation of the plasmon resonances mode, the strong local field induces an expected increase of the second-harmonic generation with conversion efficiencies 10-6-10-7. The distributions of fundamental frequency electric field and second-harmonic electric field inside the central dielectric layer region are also shown. |
| Author | Zhan, Jie Nie, Guozheng Liu, Qiong Zhou, Renlong Wu, Mengxiong Xie, Suxia Wu, Lingxi Deng, Hui |
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| Cites_doi | 10.1088/2040-8978/16/2/025002 10.1103/PhysRevLett.104.127401 10.1364/OL.34.002844 10.1088/0022-3727/45/20/205102 10.1063/1.2755780 10.1364/OE.18.018229 10.1103/PhysRevB.77.195127 10.1364/OE.19.010193 10.1063/1.3695154 10.1021/nl9041033 10.1364/OL.33.001975 10.1364/OL.39.001137 10.1007/s11082-013-9652-x 10.1103/PhysRevLett.104.153901 10.1364/OE.17.014502 10.1103/PhysRevB.79.235109 10.1364/OE.20.004856 10.1364/OE.18.007288 10.1103/PhysRevLett.109.015502 10.1088/0957-4484/24/20/205702 10.1016/j.jcp.2010.04.016 10.1021/nl1000949 10.1038/srep02358 10.1103/PhysRevLett.105.077401 10.1039/C3NR05745C 10.1364/OE.21.001606 |
| ContentType | Journal Article |
| Copyright | Copyright © 2014 Renlong Zhou et al. Copyright © 2014 Renlong Zhou et al. Renlong Zhou et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. |
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| DOI | 10.1155/2014/150957 |
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| Snippet | Second-harmonic generation in split ring resonator multilayer nanostructure is studied with the finite-difference time-domain (FDTD) method. The fundamental... Second‐harmonic generation in split ring resonator multilayer nanostructure is studied with the finite‐difference time‐domain (FDTD) method. The fundamental... |
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| SubjectTerms | Aircraft accidents & safety Dielectric constant Electric fields Finite difference method Hobbies Human error Multilayers Nanomaterials Nanostructure Replicas Resonant frequency Resonators Sensors |
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| Title | High Absorption and Second-Harmonic Generation in Split Ring Resonator Multilayer Nanostructure |
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