Metallic nano-particles for trapping light
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- Tang, Y. & Vlahovic, B. Nanoscale Res Lett (2013) 8: 65. doi:10.1186/1556-276X-8-65
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We study metallic nano-particles for light trapping by investigating the optical absorption efficiency of the hydrogenated amorphous silicon thin film with and without metallic nano-particles on its top. The size and shape of these nano-particles are investigated as to their roles of light trapping: scattering light to the absorption medium and converting light to surface plasmons. The optical absorption enhancement in the red light region (e.g., 650nm) due to the light trapping of the metallic nano-particles is observed when a layer of metallic nano-particle array has certain structures. The investigation of the light with incident angles shows the importance of the coupling efficiency of light to surface plasmons in the metallic nano-particle light trapping.
73.20.Mf, 42.25.s, 88.40.hj
KeywordsNano-particles Surface plasmons Optical absorption enhancement
H: Hydrogenated amorphous silicon
Finite difference time domain
Perfect matched layer.
There has been a growing interest in developing thin film silicon solar cells that minimize material costs and maintains high efficiency. It is because that silicon is an abundant element with almost optimal band gap and excellent junction formation characteristics, and the availability of nano-technologies makes it possible to fabricate high quality desired nano-structures. Currently, most of the solar cells are based on the crystalline silicon wafer with the thickness between 200 and 300 μm, and therefore, around 40% of the cost is the silicon wafer. Scientists proposed to develop the thin film solar cells to save the cost by decreasing the thickness of the silicon. Moreover, there is another reason to develop thin film solar cells beyond the cost, it is the absorption efficiency. Since the minority carrier diffusion length is less than or around 300 nm for amorphous silicon [1, 2, 3], it is possible to improve the absorption efficiency for a thin film solar cell. Hydrogenated alloy of amorphous silicon (a-Si:H) has higher absorption coefficient than that of the crystalline silicon. Due to this fact, in the visible part of the solar spectrum, a-Si:H absorbs almost 100 times more than crystalline silicon. In practice, the thickness of a-Si:H solar cells can be around 0.3 μm only . However, a limitation in all thin film solar cell technologies is that absorbance of red spectrum is too small, because of the indirect band gap of silicon. Therefore, one of the major driving forces in the thin film solar cell field is to structure the light-trapping (LT) schemes in order to increase absorption in the red spectrum. One traditional method is to create surface structure on top of the solar cells. However, those surface structures that were used for LT in wafer-based cells are not suitable for thin film solar cells. Since those structures were mostly pyramids with a size of 2 to 10 μm etched into the surface, they are too thick and too large for the thin film solar cells, even the wavelength-scale texture on the substrate followed by thin film solar cell on top are not suitable for thin film solar cells either.
In order to overcome these LT problems and to increase light absorption, new method based on excitation of surface plasmon  resonance via scattering from noble metal nano-structures was proposed by Catchpole and Polman . The enhancement of optical absorption and photocurrent in a semiconductor (e.g., crystalline Si) via the excitation of surface plasmon resonances in spherical Au nano-particles deposited on the semiconductor surface was reported . These enhancement in absorption within the crystalline Si results in increased photocurrent response in Si pn junction diodes over wavelength ranges that correspond closely to the nano-particle plasmon resonance wavelengths. The application of surface plasmon resonance on a-Si:H was reported  in 2006, the forward scattering surface plasmon polariton modes in Au nano-particles deposited above the amorphous silicon film improve transmission of electromagnetic radiation, and an enhancement in short-circuit current density and energy conversion efficiency in amorphous silicon p-i-n solar cells is observed. A method of enhancing light trapping by tuning localized surface plasmons through the modification of the local dielectric environment of the particle was reported  in 2009. The surface plasmon resonances can be redshifted by up to 200 nm through the modification of the local dielectric environment of the particles; the optical absorption is increased in an underlying Si wafer fivefold at a wavelength of 1,100 nm and enhances the external quantum efficiency of thin Si solar cells by a factor of 2.3 at this wavelength. The resonance frequency of metal nano-particles depends on the size, shape, particle material, and refractive index of the surrounding medium . The resonance frequency gets redshifted when the dielectric functions of the surrounding medium increase. Mokkapati et al.  presented their method for optimizing the light-trapping efficiency of periodic grating arrays of metal nano-particles for Si solar cell applications. They suggest that the pitch of the grating should be chosen to allow at least one diffraction mode propagating outside the escape cone in Si for long wavelength light.
Surface plasmons and Mie scattering
where the first term on the left hand side is the part convert from the incident light, k0 is the wave vector of it, θ is the incident angle of the light, the second term on the left hand side is the momentum from the periodic structure, n is the refractive index, and d is the period of the structure.
Mie scattering theory [13, 14] can be applied to find the optimal size of the particles, which will provide larger scattering cross-section than its geometric cross-section and even more importantly larger than its absorption cross-section. The Mie scattering is a scattering of electromagnetic waves by a sphere of radius a and permittivity ε in homogeneous systems. The scattering and absorption cross-sections are very important because they give the power that is scattered by the particle or absorbed by the particle. The scattering cross-section multiplied by the power density of the incident wave is equivalent to total amount of energy removed from the electromagnetic wave due to scatter in all directions, and a certain amount of energy is absorbed, which results in a heating of the target. The cumulative effective of scattering and absorption is the absorption cross-section.
Therefore, the absorption efficiency is . We study the size of the particles as a function of the scattering and absorption efficiency using the Mie scattering theory. One important thing to mention is that these higher plasmonic modes are followed by higher absorption which is in accordance with the observations made by .
Metallic nano-particles for LT
We calculated the efficiencies of scattering and absorption of the gold spherical particles in different sizes using the MiePlot (Philip Laven, Geneva, Switzerland) . In this calculation, we choose the sounding medium of air temperature at 25°C and the incident plane wave wavelength from 240 to 840 nm. Our study shows that for a particle with a diameter of 10 nm, which is small when compared with the wavelength, the power scattered by the particle is much less than the product of geometric cross-section and incident Poynting vector. Therefore, the scattering cross-section is much less than geometric cross-section. In other words, the efficiency of absorption is greater than the scattering efficiency of this small particle; thus, for metallic spherical nano-particle, much smaller than an incident wavelength absorption is dominant. Our calculations show that its absorption still prevails over scattering for particles with a diameter of 50 nm, but they are at the same order of magnitude (Qs ≈ 6.5 and Qa ≈ 7.8) and within a narrow spectrum from 350 to 400 nm. For particles with a diameter of 100 nm, the scattering cross-section is higher (Qs ≈ 8 and Qa ≈ 2). In this case, the scattering prevails over absorption, and more importantly, the spectrum of the scattering is much broader (300 to 500 nm) than the 50-nm diameter particles; meanwhile, the absorption spectrum is broader. This is because the higher-order plasmon modes are excited. Therefore, the higher plasmonic modes are followed by higher absorption, which is accordance with the observations in . Particles with diameters of 200 and 300 nm are investigated, too. Both particles show similar pattern with broadening the spectrum to the red light wavelength of Qs. These calculations show that the metallic nano-particle will have a broad spectrum of scattering for particles with a diameter larger than 100 nm; therefore, it is possible to enhance the absorption over a broad spectrum when the solar cell is placed beneath the metallic particles. Moreover, besides the scattering from the metallic nano-particle to the thin film, the surface plasmon of the metallic nano-particles can trap the incident lights to the thin film, too. Thus, the thin film solar cell absorption is enhanced by the metallic nano-particles in two ways: surface plasmons and scattering.
The LT of a thin film of a-Si with metallic nano-particles on its top is investigated. The metallic nano-particles are patterned on the a-Si thin film as shown in Figure 1a, where Λ is the period of the array; D and h are the side length and the height of the nano-block, respectively; t is the thickness of the a-Si thin film. We choose gold as the metal in this investigation; its optical properties are described by a dispersive complex dielectric function , and the optical properties of the a-Si are taken from Sopra N&K Database (Sopra Group, Belfast, Ireland). We applied the finite difference time domain (FDTD) software of MEEP  to simulate the metallic nano-particles on a-Si thin film. The sketch of the unit cell for the FDTD is shown in Figure 1b. A plane wave impinges on the metallic nano-particle array with an incident angle of θ. The orientation of the incidence plane is located by the azimuthally angle φ measured from the x-axis. In the simulation, the metallic array is illuminated with the plane wave normal to the metal film (at θ = 0 and φ = 0).
In these simulations, the a-Si:H thin film is sitting in the middle of a computing unit cell (shown in Figure 1b), the metallic nano-particle is placed on the a-Si thin film, and the boundary conditions of the unit cell are set as periodically (Bloch-periodic in both x and y directions). Two perfect match layers (PMLs) are put at both ends (z direction) in the unit cell. Next to the PML on the right side, a plane wave source is set to illuminate the thin film with metallic nano-particles on it, and two detectors are put into the unit cell to measure the transmission spectra by computing the fluxes of these Fourier-transformed electric fields. It is important to setup proper thickness of the PMLs to reduce numerical reflection. The thicknesses of the PMLs are dependent on the working wavelength.
Results and discussion
Optical absorption in thin a-Si:H film enhanced by metallic nano-particles was investigated by simulations. The investigation of the scattering of metallic spherical particles shows that it is possible to provide larger scattering cross-section than geometry and absorption cross-sections for particles with a diameter of 100 nm or bigger. The scattering of metallic nano-particles makes the light travel in the thin film in a longer path; therefore, higher optical absorption occurs due to more opportunities of the light to interact with the medium. Besides the scattering, the metallic nano-particles convert part of the incident light to surface plasmons, which propagate on the surface of the thin film and in the thin film. The FDTD simulations of the metallic nano-particles show that the absorption of the red spectrum is enhanced by the nano-particles (nano-blocks and nano-cylinders). For the height of 100 nm, particles have significant enhancement for red-light absorption.
Our study shows that the dominant enhancement effect comes from the surface plasmon resonance while the scattering contributed partial enhancement, and it is the main reason of using metallic particles which not only induce surface plasmons but also scatter incident light. We also study the optical absorption enhancement for incident light with an angle. It shows that the 45° incident light has better enhancement in the red light; this could be mainly because the coupling efficiency of light to the surface plasmons is higher due to the wave vector of the surface plasmons as described in Equation 1. Our study indicates that the optical absorption can be enhanced in the red spectrum with metallic particles of a high coupling efficiency from light to surface plasmon. In order to achieve this, one has to carefully select the type of metal and the structure and size of the particles.
YT works on the nano-device development at NCCU since 2006; BV is the director of CREST and works on nanotechnologies and many other areas.
Authors would like to thank the support from NSF (HRD-0833184) and the support from NASA (NNX09AV07A).
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