The Optical Response of Trapezoidal Comb-Like Nanostructures

Abstract:

Metal nanostructures can be used to control light transmission on the nanometer scale. In this paper, we propose a ladder-type comb-like metal nano-grating structure, based on optical filtering properties of the comb-like nanostructures and surface plasmon resonance effect of the metal nano-structures. The comb part of the structure is the silver nano-grating with the width of 20nm and a depth difference of 5nm between the adjacent gratings. We use the 532nm CW laser as the incident light source to study the reflective properties of the P polarized light and calculate the reflected power spectrum of the structure in three different parameters, which are the silver nano-grating, the silver-air nano-grating (silver grating are separated by air) and silver-SiO2 nano-grating. The experimental results show that the light wave oscillation modes are closely related to the comb-like structure parameters (including the depth and width) on the power spectrum. Meanwhile, we also draw conclusions that different intervention media does not change the position of the light wave oscillation modes, but only a significant effect on the reflection intensity of the different modes. Furthermore, we also noted that the depth of silver nano-gratings can affect the position of the resonance peak. As the waveguide depth of the silver nano-gratings increasing, the spacing of different modes’ oscillation peak is becoming larger. Based on the finding, we can modulate the light wave oscillation modes in a very wide spectral range. The results of this paper will promote the development of the optical filter, light wave mode selection and random laser excitation.

• Periodical: Applied Mechanics and Materials (Volumes 284-287)
• Pages: 2816-2820
• DOI: https://doi.org/10.4028/www.scientific.net/AMM.284-287.2816
• Online since: January 2013
• Authors: Yun Dong Zhang, Jin Li, Han Yang Li, Ping Yuan
• Keywords: Nano-Grating, Nanostructure, Surface Plasmon

References

[1] Z. Wu, R.L. Nelson, J.W. Haus and Q. Zhan, Opt. Lett. 33 (2008) 551-553.

[2] Y. Ye, Y. Zhou, H. Zhang and L.S. Chen, Appl. Opt. 50 (2011) 1356-1363.

[3] H.E. Went, A.P. Hibbins, J.R. Sambles, C.R. Lawrence and A.P. Crick, Appl. Phys. Lett. 77 (2000) 2789.

[4] E.S.P. Leong, Y.J. Liu, C.C. Chum, B. Wang and J.H. Teng, Appl. Phys. A 107 (2012) 127-132.

[5] S. Shinada, J. Hashizume and F. Koyama, Appl. Phys. Lett. 83 (2003) 836.

[6] N. Rotenberg, M. Betz and H.M. Driel, Phys. Rev. Lett. 105 (2010) 017402.

[7] S.S. Xiao, E. Stassen, and N.A. Mortensen, J. Nanophotonics 6 (2012) 061503.

[8] J.Y. Man, Y.T. Fan, Opt. Laser Technol. 44 (2012) 608-610.

[9] R. Melik, E. Unal, N.K. Perkgoz, B. Santoni, D. Kamstock, C. Puttlitz and H.V. Demir, IEEE J. Sel. Top. Quant. 16 (2010) 450-458.

DOI: 10.1109/jstqe.2009.2033391

[10] H.S. Lee, Y.T. Yoon, S.S. Lee, S.H. Kim and K.D. Lee, Opt. Express 15 (2007) 15457-15463.

[11] N.F. Chiu, C.W. Lin, J.H. Lee, C.H. Kuan, K.C. Wu and C.K. Lee. Appl. Phys. Lett. 91 (2007) 083114.

[12] C.H. Liu and N. Behdad, J. Appl. Phys. 111 (2012) 014906.

[13] N. Kanda, K. Konishi and M.K. Gonokami, Opt. Express 15 (2007) 11117-11125.

[14] R. Zhang, X.G. Guo, J.C. Cao and H. C. Liu, J. Appl. Phys. 109 (2011) 073110.

[15] J. Jose, F.B. Segerink, J.P. Korterik, A.G. Casado, J. Huskens, J.L. Herek and H.L. Offerhaus, J. Appl. Phys. 109 (2011) 064906.

DOI: 10.1063/1.3562142

[16] G.H. Welsh, N.T. Hunt and K. Wynne, Phys. Rev. Lett. 98 (2007) 026803.

[17] Q.Q. Gan, Z. Fu, Y.J. Ding, and F.J. Bartoli, Phys. Rev. Lett. 100 (2008) 256803.

[18] Q.Q. Gan, Y.J. Ding and F.J. Bartoli, Phys. Rev. Lett. 102 (2009) 056801.

[19] A.P. Hibbins, I.R. Hooper, M.J. Lockyear and J.R. Sambles, Phys. Rev. Lett. 96 (2006) 257402.