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Journal of Nanomaterials
Volume 2012 (2012), Article ID 156986, 6 pages
http://dx.doi.org/10.1155/2012/156986
Research Article

Performance of Silicon Nanowire Solar Cells with Phosphorus-Diffused Emitters

State Key Laboratory of Silicon Materials, Department of Materials Science and Engineering, Zhejiang University, 310027 Hangzhou, China

Received 27 April 2012; Revised 11 June 2012; Accepted 29 June 2012

Academic Editor: Xiaodong Pi

Copyright © 2012 Lingsheng Zeng 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.

Abstract

Vertical silicon nanowire (Si NW) arrays on a Si (100) substrate have been prepared by using a low-cost and facile Ag-assisted chemical etching technique. The reflectance of Si NW arrays is very low (<1%) in the spectral range from 400 to 1000 nm. By phosphorus diffusion into Si NW arrays to fabricate solar cells, the power conversion efficiency of 8.84% has been achieved. This power conversion efficiency is much higher than that of the planar cell with the similar celling technology. It is found that the efficiency of Si NW solar cells is intimately associated with their excellent antireflection property. The surface recombination of Si NWs is the main obstacle for the improvement of solar cell efficiency. The current results are helpful to the advancement of the application of Si NWs in photovoltaics.

1. Introduction

Silicon nanowires (Si NWs) have attracted much attention for photovoltaic applications because of their unique optical and electrical properties compared to bulk silicon [14]. It is known that Si NW arrays demonstrate excellent antireflection (AR) properties due to their broadband optical absorption by multiple scattering incidents [57], and therefore can be used as solar cell absorbers for trapping light [812]. Si NWs can be prepared by various methods, including chemical vapor deposition (CVD) [13, 14], physical vapor deposition (PVD) [15], and reactive ion etching (RIE) combined with lithography techniques [16, 17]. Among these, the metal-assisted chemical etching (MACE) technique [1822] is more facile and more economical to fabricate Si NW arrays since it avoids high temperature or high vacuum. Thus, solar cells based on Si NW arrays fabricated by MACE have been widely investigated [812]. Zhu’s group fabricated Si NW solar cells based on single-crystal Si substrate and polycrystalline Si substrate. They obtained the power conversion efficiency ( 𝜂 ) of 9.31% and 4.73% [8]. Later on, they fabricated solar cells based on slantingly aligned Si NWs on a Si (111) wafer and obtained improved solar cell performance [9]. Using a PSG-doped Si NW arrays as the n+ emitters and a screen-printing technique to fabricate front electrodes, the efficiency of Si NW solar cells has fallen in the range from 3.55% to 16% [12]. All these results show that despite the excellent AR property of Si NWs, the efficiency of solar cells based on Si NWs is much lower than that of conventional silicon solar cells. The main problem is the high series resistance induced by the loose contact between the electrodes and Si NW arrays.

In this work, the solar cells based on Si NW arrays have been fabricated. The phosphorus diffusion is used to form the emitters, and the metal electrodes are evaporated on the surrounding region of Si NWs with a flat surface to avoid high series resistance. It is found that the performance of Si NW arrays-based solar cells is much better than that of the solar cells based on the planar silicon due to the excellent AR property of Si NWs.

2. Experiment Details

The starting materials are p-type <100> Czochralski (CZ) silicon wafers with a resistivity of 3 Ω cm. After cleaning, the electrical tape was used to cover the back and edge of the cleaned substrates, leaving an area of 1 × 1 cm2 at the sample center. Subsequently, the samples were immersed in an aqueous solution of 4.6 M HF (40 wt%) and 0.005 M AgNO3 for 60 s to form Ag nanoparticle netlike films. These Ag-deposited wafers were etched to form the Si NWs in the mixture of 4 M HF (40 wt%) and 0.2 M H2O2 (30 wt%) solution for different time. The morphology and structure of Si NW arrays were characterized by a field-emission scanning electron microscope (SEM) (Model HITACHI S4800) and a transmission electron microscope (TEM) (Model PHILIPS cm200). Optical reflectance spectra were measured with a hitachi U-4100 UV-VIS-NIR spectrophotometer. After removing the Ag nanoparticles at the sample surface with nitric acid (65 w% HNO3), the samples were fabricated into solar cells. A standard sample without Si NWs was used as the reference. By spinning liquid POCl3 source on the sample surface, the diffusion annealing at 900°C for 20 min is used to form a spatially uniform n-emitter. The parasitic layer was removed in a diluted hydrofluoric acid solution. The front metal contacts were made by Ag thermal evaporation through a mask. The ohmic contact was formed by scratching InGa alloy at the sample backside. The schematic process for the Si NW solar cells is present in Figure 1.

156986.fig.001
Figure 1: Schematic illustration of the fabrication process for preparing Si NW arrays-based solar cells. (a) Initial p-type silicon wafer. (b) Formation of Vertical Si NW arrays on the wafer. (c) Formation of a spatially uniform n-type emitter by phosphorus diffusion. (d) Formation of electrode on the rear and front surfaces. (e) Planar schematic of the device.
156986.fig.002
Figure 2: (a) Planar image of Ag nanoparticle netlike films deposited on (100) silicon substrates. (b) The image of the planar area of the sample etched for 20 s in aqueous H2O2/HF solution. (c) Planar image of as-prepared Si NW. (d) Cross-sectional image of as-prepared Si NW. (e) Enlarged cross-sectional image of the bottom of the arrays. (f) TEM image of individual as-prepared Si NWs.

3. Results and Discussion

Figure 2(a) shows the planar image of Ag nanoparticles deposited on (100) silicon substrates via the electroless metal deposition method. It is obvious that Ag nanoparticles have formed a network. Figure 2(b) demonstrates the plan-view micrograph of the Si NWs sample after etching for 20 s in aqueous H2O2/HF solution. It can be seen that some areas of Ag are caved in, and the silicon areas protrude outward from the interspaces among the Ag nanoparticles. It indicates that the silicon parts under the Ag nanoparticles are etched off and then the shallow pits form due to the catalytic role of Ag, and the silicon uncovered with Ag remains almost unchanged. After etching for a longer time, the Si NWs can be created as the Ag nanoparticles continue to sink. Figures 2(c) and 2(d) show the planar and the cross-sectional views, respectively, of the Si NW arrays. As can be seen from the SEM micrographs, these Si nanowires are tangled with each other and hold together in bundles. This phenomenon could be caused by capillary action during the drying process due to the high aspect ratio of silicon nanowires. The diameter of silicon nanowires generally ranges from 40 to 200 nm. Note that the silver particles could be found to lie at the bottom of the Si NWs, as shown in Figure 2(e). Figure 2(f) shows the TEM micrograph of a Si NW. It indicates that the diameter of individual nanowire is roughly uniform.

Figures 3(a)3(e) demonstrates the cross-sectional SEM micrographs of Si NW arrays with different length fabricated at 0.2 M H2O2 and room temperature for 30 s, 60 s, 90 s, 120 s, and 150 s, respectively. The SEM observation clearly revealed that the lengths of the produced Si NWs increased with the etching time, ranging from 340 nm to 1700 nm, which indicates that the length of the Si NWs can effectively be tailored by prolonging the etching time. Figure 3(f) shows the Si NW length as a function of the etching time. An excellent linear behavior can be obtained. The etching rate can be evaluated to be about 11.6 nm/min.

fig3
Figure 3: Cross-sectional images and length of Si NWs etched for different time. (a) 30 s; (b) 60 s; (c) 90 s; (d) 120 s; (e) 150 s; (f) length of the Si NWs ( 𝐿 ) versus etching time ( 𝑡 ) curve.

Figure 4 shows the reflectance of Si NWs and polished wafer as a function of light wavelength. Note that the polished Si wafer has the reflectance of 35% for sun light. It can be seen that the as-grown Si NW arrays exhibit not only a large suppression of the reflectance over the entire light wavelength range, but also a very different reflection behavior from polished Si. The reflectance decreases with the wavelength increasing. The reflectance is smaller than 18%, 9%, 5%, 2%, and 1% at the nanowires length of 340 nm, 542 nm, 908 nm, 1460 nm, and 1700 nm, respectively. This can be attributed to the three important properties of Si NW arrays. One is the extremely high surface area of the Si NW arrays. The second is the suppression of the reflectance over a wide-spectral bandwidth due to the subwavelength-structured (SWS) surface of the Si NW arrays. The third is a gradual change in the refractive index with depth due to a porosity gradient throughout the Si NW arrays which closely resembles a multi-antireflection layer coating [8, 12]. It should also be mentioned that the interference peaks in the reflectance spectra of the Si NW arrays are related to the periodic nanostructure nature to some extent.

156986.fig.004
Figure 4: Reflectance of polished silicon and Si NW arrays of various length.

Figure 5 shows the illuminated I–V characteristics of the referenced cell and the Si NW cell with the Si NW length of 1700 nm. Both kinds of solar cells exhibit the diode characteristics. Note that the referenced cell has an energy conversion efficiency ( 𝜂 ) of 5.65%. The open-circuit voltage ( 𝑉 o c ), the short-circuit current density ( 𝐽 s c ), and the fill factor (FF) are 500 mV, 19.53 mA/cm2, and 0.578. However, the performance of the Si NW cells has been improved remarkably, with a better parameters of 𝜂 = 8.84%, 𝑉 o c = 500 mV, 𝐽 s c =33.40 mA/cm2, and FF =0.529. The values of 𝜂 and 𝐽 s c of the Si NW cell are enhanced by 56% and 71%, respectively, while the value of 𝑉 o c is almost the same as that of reference sample. It is obvious that the enhancement of 𝜂 mainly originates from the increase of 𝐽 s c , which attributes to the strong light trapping of Si NWs, compared with the referenced cell.

156986.fig.005
Figure 5: Illuminated current-voltage plot of control cell based on polished silicon wafer and Si NW arrays-based solar cells (of 1700 nm length).

In order to present a further verification, the external quantum efficiency (EQE) and internal quantum efficiency (IQE) are measured in the light wavelength range of 300~1100 nm, see Figure 6. Note that the IQE spectra is derived from EQE by IQE = EQE/(1− 𝑅 ), where 𝑅 represents the reflectance of solar cell. From Figure 6(a), it can be seen that the EQE of the Si NW cells is much higher than that of the referenced cell, consistent with the value of 𝐽 s c . Compared with IQE at the long wavelength demonstrated in the Figure 6(b), the IQE at the short wavelength are much lower for both of cells. This suggests that the surface recombination for photogenerated minority carriers is quite heavy for both kinds of cells. The IQEs of the Si NW cell are higher than that of the referenced cell in the long wavelength range, which means that the cell has a higher collection efficiency of minority carriers induced by long wavelength light.

fig6
Figure 6: (a) IQE and (b) EQE as a function of the wavelength for the planar solar cell and the Si NW solar cell.

Even though the Si NW arrays have an excellent AR property, the photovoltaic conversion efficiency is still much lower than that of the conventional solar cell. One of the main reasons still lies in the ultrahigh surface area of Si NWs with numerous surface defects and dangling bonds which will accelerate the surface recombination of photogenerated minority carriers. The other is lower carriers collection efficiency of the metal electrode around the area of cell than the metal grid electrode, which increases the diffusion length of photogenerated minority carriers before they are collected although it reduces the contact resistance. Therefore, good surface passivation and optimized electrode design are required to further improve the performance of Si NW array-based solar cell. In addition, some other parameters, such as Si NW arrays morphology, phosphorus diffusion, and rear electrode fabrication, should also be optimized for a higher efficiency of solar cells.

4. Conclusions

The 1 × 1  cm2 Si NW arrys on (100) Si substrate has been fabricated through a low-cost and facile Ag-assisted chemical etching technique. The lengths of the synthesized Si nanowires were found to increase linearly with etching time for silicon substrates and the Si NW arrays of longer length have lower reflectance in our investigated length range. A new method to make front electrodes on Si NW arrays-based solar cells through evaporating Ag around the area of Si NW arrays has been developed to make a compact contact. By a simple phosphorus diffusion to form the emitter in such samples, the Si NW solar cell with excellent AR property exhibits a higher power conversion efficiency of 8.84%. The analysis of reflectance and quantum efficiency suggest that the improved device performance is attributed to the excellent AR property of the Si NW arrays. To further improve the performance of Si NW arrays-based solar cell, many process parameters, for example, surface passivation, front and rear electrode design, Si NW arrays morphology, and phosphorus diffusion, should be optimized.

Acknowledgments

This work is supported by National Natural Science Foundation of China (Grant nos. 60906002 and 50832006), National Key Technology R&D Program (Grant no. 2011BAE03B13), and Innovation Team Project of Zhejiang Province (Grant no. 2009R50005).

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