Plasmonic Filters Based on Lithographically Patterned and Hexagonally Arranged Triangular Silver Nanoparticles Array

Liu, Jing; Cai, Haoyuan; Tang, Kai; Kong, Lingqi

doi:https://doi.org/10.1155/2015/195320

Advances in Materials Science and Engineering

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Research Article | Open Access

Volume 2015 | Article ID 195320 | https://doi.org/10.1155/2015/195320

Plasmonic Filters Based on Lithographically Patterned and Hexagonally Arranged Triangular Silver Nanoparticles Array

Jing Liu,^1,2Haoyuan Cai,¹Kai Tang,¹and Lingqi Kong²

Academic Editor: Rui Vilar

Received28 Sept 2014

Accepted13 Nov 2014

Published05 Jul 2015

Abstract

A plasmonic filter applied in visible regime is proposed on the basis of hexagonally arranged triangular silver nanoparticle arrays. A method using discrete dipole approximation (DDA) to aid design parameters of the silver nanoparticle arrays is adopted for the filter design and optimization on the basis of computational numerical calculation. The influence of the particle’s thickness and period on the extinction spectrum is studied using the DDA-based computational analysis. Considering the nanofabrication condition, arrays with 40 nm thickness and 230 nm period are selected and fabricated by using nanosphere lithography (NSL) technique. The experimental spectrum is basically in agreement with the theoretical spectrum derived by the DDA calculation.

1. Introduction

Plasmonic filters provide the unique capability of manipulating light at subwavelength scales by using versatile nanostructures, such as cubes [1, 2], clusters [3], shells [4], disks [5, 6], holes [7, 8], rings [9], rods [10–14], and particles with arbitrary shapes [15–17]. So far, many different types of plasmonic devices have been demonstrated, including modulators [18], interferometers [19], switches [20], polarizers [21], and absorbers [22, 23].

Plasmonic structures being used as optical filter have the following advantages [24]: the passing bandwidth is tunable through modulation of geometrical parameters and materials of the nanoparticles. This filter can work in aqueous environments such as organic chemical and biological solutions because there is no chemical reaction between the organic solution and metallic particles. This plasmonic filter is cost-effective by virtue of replication technique for device fabrication. The dimensional (2D) metallic nanoparticle arrays can also be used as a high efficiency polarization filter in the visible regime by virtue of their anisotropic response to the EM wave. Wu et al. report a metamaterial-based plasmonic filter which is applicable in terahertz [25]. The realization of the plasmonic structure in terahertz ranges may lead to some applications such as a high pass filter in the terahertz imaging systems [26]. Recent advances in experimental techniques have allowed for the fabrication of nanoparticle arrays in different shapes, patterns, and sizes [27, 28]. Many research groups can fabricate different dimensional shapes of the sphere, ellipse, stick, triangle, and prism using different fabricated methods [29].

Both the thickness and the period of the metallic nanoarrays are of particular importance for surface plasmon resonances and couplings, hence affecting photon flow accordingly. Fu et al. proposed a rhombic Ag nanoparticles array-based plasmonic filter for visible wavelength regime [24]. However, our study found that, compared with the rhombic Ag nanoarrays, hexagonally arranged triangular nanoarrays present more stable structure and optical properties, therefore being more suitable for plasmonic filters. What is more, the refractive index sensitivity (RIS) and figure of merit (FOM) strongly depend on the arrangement, the thickness, and period of the nanoarrays. We have done a further study on these two important factors. In this work, a new plasmonic filter working in visible wavelength regime is presented on the basis of hexagonally arranged triangular silver nanoparticle arrays with suitable thickness and period. DDA method is used to calculate the RIS and FOM of the nanostructure arrays with different thicknesses and periods. We develop an extended nanosphere lithography (NSL) method to fabricate the silver nanoparticle arrays with different thicknesses and periods. Our results therefore show great potential for applications in the visible wavelength regime.

2. DDA Method

The DDA provides a convenient method for describing light scattering from nanoparticles of arbitrary shape. In DDA formalism, the object of interest, usually called “target,” is described as a cubic array lattice of electric dipoles (-point dipoles) in which the polarizability and position vector of each dipole are specified as and , respectively. The induced dipole polarization in each element is determined from [30–32]where the local field is the sum of the field radiated from all the other dipoles. For a given wavelength , including the contribution of all the other dipoles, the local field can be written aswhere and are the wave vector and the amplitude of the incident radiation, respectively. The contribution to the electric field at position due to the dipole at position is contained in the second term on the right side of (2) and is normally expressed in terms of the dipole-dipole interaction matrix aswhere and correspond to the dipole-dipole position difference vector and magnitude that are defined as and , respectively. Substituting (2) and (3) into (1), we can generate the system of equationswhere the off-diagonal elements of the matrix are the same as and the diagonal elements of the matrix are .

For a system with total dipoles, , and are -dimensional vectors and is a matrix. Solving this set of complex linear equations, the polarizations are determined, and from this we can calculate cross section of the extinction as

3. Filter Design

In the DDA algorithm, we model the hexagonally arranged triangular silver nanoparticle arrays. This work highlights the problems in recent experiments, the geometrical parameters of the hexagonally arranged triangular silver nanoparticle arrays which cannot be decided by the experiment facture only. We will show that the calculation results are in quantitative agreement with those of the experiments. The computational calculation-based design method for determining the parameters of the hexagonally arranged triangular silver nanoparticle arrays from the fabrication point of view is provided.

Figures 1(a)-1(b) are schematic diagrams of the plasmonic filter. The DDA simulation-based design method for parameters determination of the silver particles is illustrated, as shown in Figure 1(c). It can be seen that the silver nanostructures have an in-plane width of 115 nm and an out-of-plane height of 40 nm. The period of the silver nanostructure arrays is 230 nm. These silver nanostructures lie in - plane and the direction of the incident light is in -axis. The polarization of the incident light is in -axis.

(a)

(b)

(c)

In our computational calculation, we consider the silver particles with the same period and in-plane widths but different out-of-plane heights which can be fabricated by depositing metal in different thicknesses through the masks after the NSL process. The calculations are carried out for the particles arranged in a triangular structure. However, the fabricated particles may have a varied thickness/height from the design value due to fabrication error. Hence it is necessary to analyze the influence of varied thicknesses on optical performance firstly. To study this point, we calculate the extinction spectra, RIS as well as FOM of the triangular Ag nanostructure arrays with different Ag layer thicknesses. The thicknesses of triangular array structure are 30, 35, 40, and 45 nm with fixed period of 230 nm. According to the calculated extinction spectra presented in Figure 2, when the Ag layer thickness increases, the intensity of the extinction and the full width at half-maximum (FWHM) decrease obviously. The positions of the peak wavelengths locate at wavelength of 691 nm, whether the thickness is 35 nm, 40 nm, or 45 nm.

(a)

(b)

In order to investigate the effect of the Ag layer thickness on the sensitivity of the nanostructure array, we calculate the extinction spectra of the effective refractive index of the medium surrounding the nanostructure array. The RIS is defined as [33], where and denote the peak of the wavelength change and the refractive index change, respectively. For the nanostructure array with 30 nm thickness of Ag layer, the peak wavelength has a red shift when the refractive index increases as shown in Figure 3(a). For example, when the refractive index increases from 1.0 to 1.05, the peak wavelength shifts from 704 nm to 730 nm, exhibiting a refractive index sensitivity of 556 nm/RIU (refractive index unit), as indicated in Figure 3(b). Figure 3(c) shows the RIS of the nanostructure arrays with different Ag layer thicknesses. The result shows that the RIS increases as the thickness of Ag layer increases from 30 to 40 nm and then decreases with further increase of Ag layer thickness to 45 nm. When the Ag layer thickness is 40 nm, the structure is very sensitive for the refractive index from 1.0 to 1.2.

(a)

(b)

(c)

The FOM for a metal nanostructure is defined as [34], where and denote the RIS and FWHM, respectively. According to Figures 2(b) and 3(c), we calculate the FOM and the calculation result is shown in Figure 4. It can be seen from Figure 4 that the FOM of the nanostructure array remains at a more stable and relatively high value, when the thickness of Ag layer increases from 40 to 45 nm.

In our calculation, the diverse diameters of the polystyrene spheres (PS) being used in fabrication are considered to adjust the period of the triangular silver particles. The correct direction for the facture of the hexagonally arranged triangular silver nanoparticle arrays is offered by means of analyzing variation of the particle periods. The period effects of the extinction spectra with fixed thickness of silver, 40 nm, are calculated by changing the periods to be 230 nm, 280 nm, 380 nm, and 460 nm, respectively. Figure 5 shows the resulting spectra, which look very similar to each other. The relationship between the FWHM and the period of the triangular silver particles is shown in Figure 5(b). When the periods are 230 nm, 280 nm, and 380 nm, the positions of the peak wavelengths are located in 691 nm. Figure 6 shows the RIS of the nanostructure arrays with different periods. Figure 7 shows the FOM of the nanostructure arrays with different periods. As can be seen from Figure 5 to Figure 7, when the period of the nanostructure array is changed to 230 nm, the extinction efficiency has a relatively higher value and the corresponding FWHM of the spectrum is the widest in the periods of 280 nm, 380 nm, and 460 nm. We can find that the nanostructure array has maximum RIS and FOM, when the period is increased from 230 nm to 280 nm. From the calculated results, we can find that the 40 nm thickness with 230 nm period is the suitable structure parameter for our calculation.

(a)

(b)

4. Filter Fabrication

Considering capability of the nanostructure fabrication in experiment, the thickness is selected as 30–45 nm and the period is selected as 230–460 nm, respectively, in the DDA calculation.

In our experiments, the triangular metal nanostructures with different thicknesses and periods are fabricated by means of NSL technique. The PS with a mean diameter of 230 nm, 280 nm, 380 nm, and 460 nm and a concentration of 10 wt% in solution are purchased from Suzhou Nano-Micro Bio-Tech Co. Ltd. First of all, close-packed nanosphere is a prerequisite. The regular monolayer as a deposition mask is principal to achieve large-area hexagonal structure. To begin with, the PS solution is diluted to be 3 wt% with deionized water. The glass substrates are thoroughly cleaned, in toluene, acetone, and ethanol for 10 min, respectively, then in piranha solution (H₂SO₄ : H₂O₂ = 3 : 1) for 2 hours to remove organic residues. To achieve a hydrophilic surface, the glass substrates are ultrasonically bathed in NH₄OH, H₂O₂, and H₂O solution with the ratio of 1 : 1 : 5 for 2 hours. Every sonication followed rinsing with large amount of deionized water. The cleaned substrates are stored in deionized water until being used.

A single-layer of size-monodisperse PS nanospheres was drop-coated onto the substrate followed by the deposition of a silver film, as shown in Figure 8.

The deposition of metallic layer (3N Ag) is performed in a home-built thermal evaporator at a pressure of 5.0 × 10⁻⁴ Pa. The substrates are rotated at speeds of 16.5 rpm all through the deposition. To achieve homogeneous deposition, the power for heating up of the source materials is carefully increased. The deposition rate is ~2.5 nm/s for silver layer. The thickness had been monitored using a Dektak 3 Series surface profiler to achieve an identical depth for a low reflectance. It is controlled to be 30, 35, 40, and 45 nm for silver films, respectively. The PS spheres are lifted off by immersing in absolute ethanol for about 5 s. The PS spheres are removed by sonication (B3500S-MT, Branson, 140 W, 42 kHZ) in absolute ethanol. Nanostructures of the achieved PS mask and the silver nanoparticle arrays are characterized by LEO-1530 SEM. Ultraviolet-visible (UV-vis) mirror reflection spectra are obtained on a Varian Cary 5000 UV-Vis-NIR spectrophotometer.

5. Results and Discussion

Figure 9 shows the SEM images of silver nanoparticle arrays for different thicknesses with fixed period of 230 nm. As shown in Figure 9(a), the silver nanoparticles exhibit a hexagonally arranged disc structure rather than triangular structure, as the thickness of deposited silver film is 30 nm. When the silver particles arrive at the glass substrate after passing through the triangular gaps, the energy falls sharply. In this case, the disc structure is easier formed because of its smaller surface energy. Besides, as the prior deposition particle has been combined with the substrate and no subsequent particle proceeds, the smaller disc structure cannot spread out into the triangular one. However, as the deposited film thickness increases, the angular structure mounts and tends to regular, which is presented as in Figures 9(b) and 9(c). As shown in Figure 9(c), the angular structure turns into regular, and its tip becomes sharp. This structure is very conducive to further modification experiments for signal detection. Figure 9(d) shows the SEM image of silver nanoparticle arrays with the silver film of 45 nm thickness. In this case, the triangular array is evident. However, the triangular tips are not as sharp as those shown in Figure 9(c), and the array is not so regular as well. This is mainly because of the deposition time, which determines the thickness of the film. Firstly, the evaporation silver particles cover the gap interspaces among the spheres, and the energy reduces greatly. Secondly, the subsequent particles combine with the advanced ones to form larger particles. Thirdly, when more and more particles accumulate, they may collapse in the triangular gaps. As their energy in the second process has decreased, the collapsed particles cannot combine with the substrate furthermore. So the particles cannot spread out into the regular triangular array, which is shown in Figure 9(d).

(a)

(b)

(c)

(d)

Different-sized silver nanoparticle arrays are presented, as shown in Figures 10(a)–10(d). The silver film thickness is fixed on 40 nm. The nanoparticles exhibit a triangular structure and are arranged as a hexagonal array on the scale of several micrometers in lateral size. When the period is 230 nm, the nanoparticles exhibit a triangular structure but that is more uniform than the other cases, the angular structure turns into regular, and its tip becomes sharp, as shown in Figure 10(a). This structure is very conducive to further modification experiments for signal detection.

(a)

(b)

(c)

(d)

Table 1 shows that the actual height of the nanoparticle varies with the thickness of the deposition film. As shown in Table 1, the thicknesses of the silver film of 30 nm, 35 nm, 40 nm, and 45 nm are experimental parameter according to the thermal evaporation conditions, while the actual heights of silver nanoparticles are gotten by the sample measurement. It is clear that as the thickness of the silver film is altered from 30 nm to 45 nm, the actual thicknesses of the silver nanoparticle are 35 nm, 37 nm, 38 nm, and 40 nm, respectively. It indicates that as the silver film thickness increases, the actual height increases gradually as well. Furthermore, the nanoparticle height increases sharply when the deposited film is thin and then tends to grow slowly as the evaporation proceeds.

In our experiments, we detected the extinction efficiency of the representative triangular silver nanoparticle array with 230 nm period and 40 nm thickness of the silver particles. The experimental and the calculated results are shown in Figure 7. It can be seen apparently that when the wavelength is 663 nm, the extinction efficiency reaches to a maximum value (Figure 11). When DDA calculation is taken to calculate the extinction efficiency, the maximum wavelength of extinction efficiency is 691 nm. The calculated result of the plasmon wavelength with the designed model agrees with recent experimental result. The only major difference with the experiment is that the experimental peak is shifted by 28 nm to the blue compared to the calculated result. This is likely caused by substrate effect (see [35]). The other reason [24] is that fabrication error caused uniformity issue for both size and shape of the particles. In addition, in DDA calculated model, the edge of the triangular nanoparticles is straight while in experiment it is curving.

Most of the results presented here are analysis and characterization of the thickness variation and array period. The results for the 2D hexagonally arranged triangular silver nanoparticle arrays show that there are suitable parameters for our experimental fabrication which are thickness of 40 nm and the period of 230 nm. The experimental results are generally in agreement with the calculated results.

6. Summary

A hexagonally arranged triangular silver nanoparticles array-based plasmonic filter is proposed for visible wavelength regime. A DDA algorithm-based design method is presented. After fabrication using NSL technique, spectroscopic results show that the measured spectrum is basically in agreement with the theoretical spectrum derived by the DDA calculation. Therefore, its application in the visible wavelength regime is possible.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This work was supported by Science and Technology Plan Projects of Xiamen City under Grant no. 2013S0335/3502Z20143020 and Science and Technology Plan Projects of Fujian Provincial Science and Technology Department under Grants nos. 11151042 and 2014H0036; Science and Technology Plan Projects of Fujian Province Support The Armed Forces under Grant No. 2015.

References

H. J. Chen, Z. H. Sun, W. H. Ni et al., “Fano resonance in (gold core)-(dielectric shell) nanostructures without symmetry breaking,” Small, vol. 5, pp. 2111–2119, 2009.
View at: Google Scholar
X. Kou, Z. Sun, Z. Yang, H. Chen, and J. Wang, “Curvature-directed assembly of gold nanocubes, nanobranches, and nanospheres,” Langmuir, vol. 25, no. 3, pp. 1692–1698, 2009.
View at: Publisher Site | Google Scholar
J. A. Fan, C. Wu, K. Bao et al., “Self-assembled plasmonic nanoparticle clusters,” Science, vol. 328, no. 5982, pp. 1135–1138, 2010.
View at: Publisher Site | Google Scholar
J. B. Lassiter, J. Aizpurua, L. I. Hernandez et al., “Close encounters between two nanoshells,” Nano Letters, vol. 8, no. 4, pp. 1212–1218, 2008.
View at: Publisher Site | Google Scholar
I. Zorić, E. M. Larsson, B. Kasemo, and C. Langhammer, “Localized surface plasmons shed light on nanoscale metal hydrides,” Advanced Materials, vol. 22, no. 41, pp. 4628–4633, 2010.
View at: Publisher Site | Google Scholar
Y. J. Liu, Y. B. Zheng, J. Liou, I.-K. Chiang, I. C. Khoo, and T. J. Huang, “All-optical modulation of localized surface plasmon coupling in a hybrid system composed of photoswitchable gratings and au nanodisk arrays,” The Journal of Physical Chemistry C, vol. 115, no. 15, pp. 7717–7722, 2011.
View at: Publisher Site | Google Scholar
T. W. Ebbesen, H. J. Lezec, H. F. Ghaemi, T. Thio, and P. A. Wolff, “Extraordinary optical transmission through sub-wavelenght hole arrays,” Nature, vol. 391, no. 6668, pp. 667–669, 1998.
View at: Publisher Site | Google Scholar
Y. J. Liu, E. S. P. Leong, B. Wang, and J. H. Teng, “Optical transmission enhancement and tuning by overylaying liquid crystals on a gold film with patterned nanoholes,” Plasmonics, vol. 6, no. 4, pp. 659–664, 2011.
View at: Publisher Site | Google Scholar
A. R. Halpern and R. M. Corn, “Lithographically patterned electrodeposition of gold, silver, and nickel nanoring arrays with widely tunable near-infrared plasmonic resonances,” ACS Nano, vol. 7, no. 2, pp. 1755–1762, 2013.
View at: Publisher Site | Google Scholar
H. Chen, L. Shao, Q. Li, and J. Wang, “Gold nanorods and their plasmonic properties,” Chemical Society Reviews, vol. 42, no. 7, pp. 2679–2724, 2013.
View at: Publisher Site | Google Scholar
Y. Zheng, M. Xiao, S. Jiang, F. Ding, and J. Wang, “Coating fabrics with gold nanorods for colouring, UV-protection, and antibacterial functions,” Nanoscale, vol. 5, no. 2, pp. 788–795, 2013.
View at: Publisher Site | Google Scholar
G. A. Wurtz, R. Pollard, W. Hendren et al., “Designed ultrafast optical nonlinearity in a plasmonic nanorod metamaterial enhanced by nonlocality,” Nature Nanotechnology, vol. 6, no. 2, pp. 107–111, 2011.
View at: Publisher Site | Google Scholar
G. A. Wurtz, W. Dickson, D. O'Connor et al., “Guided plasmonic modes in nanorod assemblies: strong electromagnetic coupling regime,” Optics Express, vol. 16, no. 10, pp. 7460–7470, 2008.
View at: Publisher Site | Google Scholar
D. P. Lyvers, J.-M. Moon, A. V. Kildishev, V. M. Shalaev, and A. Wei, “Gold nanorod arrays as plasmonic cavity resonators,” ACS Nano, vol. 2, no. 12, pp. 2569–2576, 2008.
View at: Publisher Site | Google Scholar
A. M. Kern and O. J. F. Martin, “Excitation and reemission of molecules near realistic plasmonic nanostructures,” Nano Letters, vol. 11, no. 2, pp. 482–487, 2011.
View at: Publisher Site | Google Scholar
J. P. Kottmann, O. J. F. Martin, D. R. Smith, and S. Schultz, “Spectral response of plasmon resonant nanoparticles with a non-regular shape,” Optics Express, vol. 6, no. 11, pp. 213–219, 2000.
View at: Publisher Site | Google Scholar
A. Lovera and O. J. F. Martin, “Plasmonic trapping with realistic dipole nanoantennas: analysis of the detection limit,” Applied Physics Letters, vol. 99, no. 15, Article ID 151104, 2011.
View at: Publisher Site | Google Scholar
J. A. Dionne, K. Diest, L. A. Sweatlock, and H. A. Atwater, “PlasMOStor: a metal-oxide-Si field effect plasmonic modulator,” Nano Letters, vol. 9, no. 2, pp. 897–902, 2009.
View at: Publisher Site | Google Scholar
Y. K. Gao, Z. M. Xin, Q. Q. Gan, X. H. Cheng, and F. J. Bartoli, “Plasmonic interferometers for label-free multiplexed sensing,” Optics Express, vol. 21, no. 5, pp. 5859–5871, 2013.
View at: Publisher Site | Google Scholar
Y. J. Liu, Q. Hao, J. S. T. Smalley, J. Liou, I. C. Khoo, and T. J. Huang, “A frequency-addressed plasmonic switch based on dual-frequency liquid crystals,” Applied Physics Letters, vol. 97, no. 9, Article ID 091101, 2010.
View at: Publisher Site | Google Scholar
Y. Zhao, M. A. Belkin, and A. Alù, “Twisted optical metamaterials for planarized ultrathin broadband circular polarizers,” Nature Communications, vol. 3, pp. 870–879, 2012.
View at: Publisher Site | Google Scholar
K. Aydin, V. E. Ferry, R. M. Briggs, and H. A. Atwater, “Broadband polarization-independent resonant light absorption using ultrathin plasmonic super absorbers,” Nature Communications, vol. 2, pp. 517–524, 2011.
View at: Google Scholar
Y. Zhao, Q. Hao, Y. Ma et al., “Light-driven tunable dual-band plasmonic absorber using liquid-crystal-coated asymmetric nanodisk array,” Applied Physics Letters, vol. 100, no. 5, pp. 053119–053126, 2012.
View at: Publisher Site | Google Scholar
Y. Q. Fu, S. L. Zhu, X. L. Zhou, and W. Zhao, “Rhombic silver nanoparticles array-based plasmonic filter,” International Journal of Modern Physics B, vol. 25, no. 19, pp. 2557–2566, 2011.
View at: Publisher Site | Google Scholar
D. Wu, N. Fang, C. Sun et al., “Terahertz plasmonic high pass filter,” Applied Physics Letters, vol. 83, no. 1, pp. 201–203, 2003.
View at: Publisher Site | Google Scholar
V. M. Lubecke, K. Mizuno, and G. M. Rebeiz, “Micromachining for terahertz applications,” IEEE Transactions on Microwave Theory and Techniques, vol. 46, no. 11, pp. 1821–1831, 1998.
View at: Publisher Site | Google Scholar
R. F. W. Pease, “Nanolithography and its prospects as a manufacturing technology,” Journal of Vacuum Science & Technology B, vol. 10, pp. 278–285, 1992.
View at: Google Scholar
J. Melngailis, A. A. Mondelli, I. L. Berry III, and R. Mohondro, “A review of ion projection lithography,” Journal of Vacuum Science and Technology B: Microelectronics and Nanometer Structures, vol. 16, no. 3, pp. 927–957, 1998.
View at: Publisher Site | Google Scholar
J. C. Hulteen, D. A. Treichel, M. T. Smith, M. L. Duval, T. R. Jensen, and R. P. Van Duyne, “Nanosphere lithography: size-tunable silver nanoparticle and surface cluster arrays,” Journal of Physical Chemistry B, vol. 103, no. 19, pp. 3854–3863, 1999.
View at: Publisher Site | Google Scholar
R. Jin, Y. Cao, C. A. Mirkin, K. L. Kelly, G. C. Schatz, and J. G. Zheng, “Photoinduced conversion of silver nanospheres to nanoprisms,” Science, vol. 294, no. 5548, pp. 1901–1903, 2001.
View at: Publisher Site | Google Scholar
B. T. Draine and P. J. Flatau, “Discrete-dipole approximation for scattering calculations,” Journal of the Optical Society of America A: Optics and Image Science, and Vision, vol. 11, no. 4, pp. 1491–1499, 1994.
View at: Publisher Site | Google Scholar
B. T. Draine and P. J. Flatau, User Guide for the Discrete Dipole Approximation Code DDSCAT.7.3.0, 2008.
S. Zhu, C. Du, and Y. Fu, “Localized surface plasmon resonance-based hybrid Au-Ag nanoparticles for detection of Staphylococcus aureus enterotoxin B,” Optical Materials, vol. 31, no. 11, pp. 1608–1613, 2009.
View at: Publisher Site | Google Scholar
L. J. Sherry, S.-H. Chang, G. C. Schatz, R. P. Van Duyne, B. J. Wiley, and Y. Xia, “Localized surface plasmon resonance spectroscopy of single silver nanocubes,” Nano Letters, vol. 5, no. 10, pp. 2034–2038, 2005.
View at: Publisher Site | Google Scholar
C. Chaumet, A. Rahmani, and G. W. Brvant, “Generalization of the coupled dipole method to periodic structures,” Physical Review B, vol. 67, pp. 165404–165411, 2003.
View at: Google Scholar

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Copyright © 2015 Jing Liu 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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