Design and fabrication of a SiOx/ITO double-layer anti-reflective coating for heterojunction silicon solar cells
Introduction
The heterojunction silicon solar cell is attracting more and more attention in both photovoltaic research and industry. The reason is that the heterojunction silicon solar cell has high efficiency [1], [2], lower thermal budget, shorter processing time, and potentially lower processing cost compared to the conventional diffused homojunction crystalline silicon (c-Si) solar cell [3]. As is the case for homojunction silicon solar cells, there are also optical losses such as reflection losses and metallic shading losses in heterojunction cells. The high refractive index of the hydrogenated amorphous silicon (a-Si:H) emitter in the heterojunction cell and the c-Si emitter in the homojunction cell results in high reflection losses (>40% in the wavelength range from 300 to 1200 nm). Therefore, anti-reflection measures are very important for reducing reflection losses and increasing the light absorption in c-Si. In the case of homojunction silicon solar cells, silicon nitride is normally used as anti-reflective (AR) coating. For heterojunction silicon solar cells, the transparent indium tin oxide (ITO) front contact layer is also designed for this AR purpose.
For the heterojunction silicon solar cell, ITO can absorb light in the ultraviolet regime due to its large band gap as well as in the infrared regime due to its free carrier absorption. In addition the high absorption coefficient of a-Si:H leads to high absorption in these thin layers at wavelengths shorter than 700 nm, further contributing to the parasitic absorption losses [4]. These absorption losses can reduce the benefits gained from the AR coating, making the design of an AR coating more complicated for a c-Si homojunction cell. In 2012, Holman et al. showed that how ITO, and p-type and intrinsic a-Si:H layers in the front side of the heterojunction silicon solar cell contribute to the current losses by comparing EQE and simulated absorption in c-Si of different solar-cell structures at wavelengths from 300 to 600 nm [5]. They concluded that no light was absorbed in ITO and p-type a-Si:H contributes to the photocurrent, whereas 20–50% of the light absorbed in intrinsic a-Si:H can contribute to this current. In this contribution, we present an accurate optical analysis of heterojunction silicon solar cells in the wavelength range from 300 nm to 1200 nm. Based on our optical analysis, we show that for AR coating design the short-circuit current density (Jsc) can be maximized by optical simulations alone, provided that the c-Si wafer absorbance is maximized since this absorbance dominates the Jsc. We show that this procedure is more accurate than simply minimizing the reflectance due to the influence of parasitic absorption of front layers. In this contribution, we illustrate this approach for designing a double-layer AR coating of both a flat and textured heterojunction silicon solar cell. In order to validate our model, solar cells with the optimized AR coating are fabricated.
Section snippets
Experimental
The structure and layer thicknesses of the heterojunction silicon solar cells with single and double layer AR coating that we process in our facility are shown in Fig. 1. The same structure is also used for simulations using ASA computer software [6], [7]. The area of the solar cells is 0.16 cm2. For the solar cells, n-type c-Si (111) FZ wafers are used with a thickness of about 280 µm and selected from a batch with resistivity between 2 and 5 Ω cm. On the back side of the c-Si wafer, a 9 nm thick
Results and discussion
In order to compare the effectiveness of an AR coating on a solar cell, it is important to take the AM 1.5 solar spectrum into account. For this investigation we have chosen the wavelength range from 300 nm to 1200 nm of the solar spectrum. The reason is that for wavelengths shorter than 300 nm, the spectral power density in the AM 1.5 spectrum is almost zero, while photons with wavelengths longer than 1200 nm are hardly absorbed by the c-Si. In this work, we define the weighted average reflectance
Conclusion
In this contribution, we present optical simulations for flat and textured heterojunction silicon solar cells with our ASA software. Our simulations show excellent agreement with reflectance measurements on real devices, indicating the accuracy of the model used. We have shown that optical optimization of textured heterojunction solar cells needs to be carried out especially in relation to the and not in relation to the since parasitic absorption plays an important role. Based on this
Acknowledgments
The work is funded by Energy Research Centre of The Netherlands. We would like to thank M. Tijssen and S. Heirman for their technical support. We also would like to thank H. Tan, J. Meerwijk, D. Deligiannis and other colleagues for their helpful discussion.
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