No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
The full text of this article is not currently available.
Actively controlled plasmonic Bragg reflector based on a graphene parallel-plate waveguide
4.B. Wang and G. P. Wang, Appl. Phys. Lett. 87(7), 013107:1-3 (2005).
10.L. Zhou, X. Q. Yu, and Y. Y. Zhu, Appl. Phys. Lett. 89(5), 051901:1-3 (2006).
14.S. A. Maier, Plasmonics: Fundamentals and Applications (Springer, 2007).
21.Z. Fang, Y. Wang, A. E. Schlather, Z. Liu, P. M. Ajayan, F. J. García de Abajo, P. Nordlander, X. Zhu, and N. J. Halas, Nano Lett. 14(1), 299–304 (2014).
23.B. Vasić, G. Isić, and R. Gajić, Appl. Phys. Lett. 113(1), 013110 (2013).
26.B. Wang, X. Zhang, X. Yuan, and J. Teng, Appl. Phys. Lett. 100(13), 131111:1-3 (2012).
30.D. Joannopoulos, S. G. Johnson, J. N. Winn, and R. D. Meade, Photonic Crystals: Molding the Flow of Light, 2nd ed. (Princeton University Press, Princeton NJ, 2008).
Article metrics loading...
We investigate theoretically and numerically a graphene parallel-plate waveguide structure with two alternate chemical potentials (which can be realized by alternately applying two biased voltages to graphene). A plasmonic
Bragg reflector can be formed in infrared range because of the alternate effective refractive indexes of SPPs propagating along graphene sheets. By introducing a defect into the Bragg reflector, and then the defect resonance mode can be formed. Thanks to the tunable permittivity of graphene by bias voltages, the central wavelength and bandwidth of SPPs stop band, and the wavelength of the defect mode can be tuned.
Full text loading...
Most read this month