Three-Terminal Amorphous Silicon Solar Cells

Tai, Cheng-Hung; Lin, Chu-Hsuan; Wang, Chih-Ming; Lin, Chun-Chieh

doi:https://doi.org/10.1155/2011/813093

International Journal of Photoenergy

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Abstract Introduction Results and Discussion Acknowledgments References Copyright Related Articles

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Thin-Film Photovoltaics 2011

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Research Article | Open Access

Volume 2011 | Article ID 813093 | https://doi.org/10.1155/2011/813093

Three-Terminal Amorphous Silicon Solar Cells

Cheng-Hung Tai,¹Chu-Hsuan Lin,¹Chih-Ming Wang,¹and Chun-Chieh Lin²

Academic Editor: Vincenzo Augugliaro

Received15 Jun 2011

Accepted05 Sept 2011

Published30 Nov 2011

Abstract

Many defects exist within amorphous silicon since it is not crystalline. This provides recombination centers, thus reducing the efficiency of a typical a-Si solar cell. A new structure is presented in this paper: a three-terminal a-Si solar cell. The new back-to-back p-i-n/n-i-p structure increased the average electric field in a solar cell. A typical a-Si p-i-n solar cell was also simulated for comparison using the same thickness and material parameters. The 0.28 μm-thick three-terminal a-Si solar cell achieved an efficiency of 11.4%, while the efficiency of a typical a-Si p-i-n solar cell was 9.0%. Furthermore, an efficiency of 11.7% was achieved by thickness optimization of the three-terminal solar cell.

1. Introduction

Amorphous silicon (a-Si) for photovoltaic applications can be deposited using the techniques of plasma-enhanced chemical vapor deposition (PECVD) [1–3], catalytic CVD (Cat-CVD) [4, 5], photo-CVD [6, 7], sputtering [8], and so forth. Since it is usually deposited at a low temperature, low-cost or flexible materials like glass, plastic, or stainless steel can be adopted as the substrate. Amorphous Si also has the advantages of an abundant supply on the earth and a high-absorption coefficient at visible wavelengths [9, 10]. These advantages make it promising for applications in thin-film photovoltaics. Amorphous Si can be applied to many types of solar cells, such as single-junction [11, 12], multijunction [13, 14], and HIT [15] (heterojunction with intrinsic thin layer) solar cells. In 2000, the stable efficiency of a single-junction a-Si solar cell (area of 1 cm²) was 9.0% [16]. In 2009. a single-junction a-Si solar cell has achieved an efficiency of 10.1% [17]. Multijunction solar cells were usually able to achieve higher efficiencies. For example, the stable efficiency of a triple-junction solar cell (a-Si/a-Si/a-SiGe tandem solar cell) was 12.1% [18], and the efficiencies of micromorph Si solar cells (a-Si/μc-Si tandem solar cells) were larger than 11% [19–21]. Multijunction solar cells are composed of two or more subcells. The working mechanism of multijunction solar cells is by way of tunnel-recombination junctions, and the final efficiency is limited by the smallest photogenerated current among all subcells [22]. This is because each subcell of a multijunction solar cell must pass through the same current. Therefore, the defects inside the a-Si may reduce the efficiencies of solar cells whether for a single-junction cell or a multijunction cell. The efficiencies are reduced due to the recombination of photogenerated carriers via defects [23, 24]. In addition, carrier mobility in a-Si is quite low. Hence, the efficiencies of typical a-Si-based solar cells are limited.

We have designed and simulated a new structure of a three-terminal a-Si p-i-n/n-i-p solar cell. The new structure enhances the electric field in a-Si solar cells and reduces the recombination rate of photogenerated carriers in order to increase the efficiency. The three-terminal device structure also avoids the effect of current mismatch between subcells [25]. In this paper, we compare the two-terminal a-Si p-i-n solar cell (control cell) and the new three-terminal a-Si p-i-n/n-i-p solar cell with the same thickness and material parameters.

2. Device Structure

Figure 1 shows the device structures and doping concentrations of the single-junction a-Si p-i-n solar cell (labeled as control) and the three-terminal a-Si p-i-n/n-i-p solar cell (labeled as three terminal). The simulation was carried out with the commercial simulation tool, ISE TCAD. The device structure and performance of the control cell were based on those in [16]. Sunlight irradiated the cells from the top of the device. In our simulation, all of the p-layers and n-layers had a thickness of 0.01 μm, and both the control cell and the three-terminal cell were 0.28 μm.

In order to contact “contact:sub” in the three-terminal solar cell, we should set the width of the subcell D-2 (see the definition in Figure 1) to be smaller than the width of the subcell D-1. Then, “contact:sub” could connect to the outer circuit. For a large area solar cell, the ratio of the contact region of “contact:sub” to the total area would be very small, and the influence due to the width decrease of the subcell D-2 could be neglected. On the other hand, the top “contact:gate” and bottom “contact:gate” of the three-terminal cell were joined and acted as the other terminal to the outer circuit.

For the control cell, most of the depletion region was in the intrinsic layer (i-layer). The photogenerated carriers were separated by an electric field of the depletion region and the electrons drifted to the “contact:sub,” while the holes drifted to the “contact:gate”. For the three-terminal cell, there are i-layers both in subcells D-1 and D-2. As with the control cell, most of the depletion region was in the i-layers. It is worth noting that the directions of the electric field in D-1 and D-2 are reversed. All of the photogenerated electrons in the three-terminal cell will drift to “contact:sub.” The photogenerated holes in D-1 will drift to the top “contact:gate,” and the photogenerated holes in D-2 will drift to the bottom “contact:gate.”

3. Results and Discussion

The key role in improving the efficiency of the three-terminal cell is the electric field in the i-layers. For a two-terminal cell, the built-in potential is distributed across the 0.28 μm-thick p-i-n structure. For a three-terminal cell, the same magnitude of the built-in potential is distributed across both the top p-i-n and bottom n-i-p structures. Hence, the average electric field of the three-terminal cell is larger than the control cell.

Figure 2 gives the I-V characteristics of the control cell and the three-terminal cell. In [16], the stable efficiency of a single-junction thin a-Si : H p-i-n solar cell was 9.0%, the short-circuit current density () was 15.8 mA/cm², and the open-circuit voltage () was 0.87 V. For the control cell in our simulation, the efficiency was 9.0%, the was 15.2 mA/cm², and the was 0.91 V. It was proved that our simulation results were close to the practical conditions. For the three-terminal cell, the efficiency was 11.4%, the was 16.5 mA/cm², and the was 0.92 V. The efficiency of the three-terminal a-Si solar cell was remarkably increased. A larger average electric field in the three-terminal cell could decrease the recombination of photogenerated carriers, and so that the efficiency was enhanced.

Figure 3 shows the generation rate (1/(cm³·s)) and recombination rate (1/(cm³·s)) of the control cell and the three-terminal cell. It could be observed that the control cell and the three-terminal cell had the same generation rate, but the three-terminal cell had a lower recombination rate than the control cell. The integral of the recombination rate over the depth was the amount of total bulk recombination. The integrals were (1/(cm²·s)) and (1/(cm²·s)) for the three-terminal cell and the control cell, respectively. The three-terminal cell had a smaller total bulk recombination, and so the efficiency of the three-terminal solar cell was higher than the control solar cell.

Figure 4 shows the band-edge diagram of the control cell and the three-terminal cell when sunlight irradiated from the left side of the band-edge diagram. With this band-edge diagram, it could be understood that, in the control cell, the photogenerated electrons would drift to the n-layer and the photogenerated holes would drift to the p-layer. In the control cell, “contact:sub” acted as the negative electrode of the solar cell, and “contact:gate” acted as the positive electrode. In the three-terminal cell, all of the photogenerated electrons would drift to the n-layer and connect to the outer circuit via “contact:sub” between the two n-layers. The photogenerated holes in the subcell D-1 would drift to the top p-layer and connect to the outer circuit via the top “contact:gate” on the top surface. The photogenerated holes in the subcell D-2 would drift to the bottom p-layer and connect to the outer circuit via the bottom “contact:gate.” Then, the top “contact:gate” and the bottom “contact:gate” were joined by metals. The directions of the photogenerated carrier flows of the three-terminal cell and the outer circuit were shown in Figure 5. Similar to the control cell, “contact:sub” in the three-terminal cell acted as the negative electrode, and two “contact:gates” acted as the positive electrode.

The thicknesses of the subcell D-1 and the subcell D-2 of the previous three-terminal cell were both 0.14 μm. We optimized the three-terminal cell by adjusting the thickness of the subcell D-1 and the subcell D-2 (Figure 6). First, we kept the thickness of the subcell D-2 at 0.14 μm and adjusted the thickness of the subcell D-1 from 0.06 μm to 0.32 μm. We obtained the highest efficiency when the thickness of the subcell D-1 was 0.14 μm. Therefore, the thickness of the subcell D-1 was kept at 0.14 μm, and the thickness of the subcell D-2 was adjusted from 0.06 μm to 0.32 μm. The thicker the subcell D-2, the higher the efficiency. The efficiency almost saturated as the thickness became greater than 0.24 μm. From the simulation results, we obtain the following conclusions: (I) as the thickness of the subcell D-2 is fixed and the thickness of subcell D-1 is smaller than 0.14 μm, a thinner subcell D-1 will produce a lower in the three-terminal cell as a result of insufficient absorption, thus leading to a lower efficiency; (II) the thicker the subcell D-1, the greater the overall , but the lower the overall . Therefore, the efficiency decreases if this subcell is too thick (thicker than 0.14 μm). The reason for decreasing in the overall as the thickness increases is discussed as follows. When the subcell D-1 is too thick, most of sunlight is absorbed by the subcell D-1, which leads to the decrease in absorption in the subcell D-2. This reduces the photogenerated current in the subcell D-2, and therefore the subcell D-2 has a lower than the subcell D-1. For a three-terminal cell, subcells D-1 and D-2 are connected in parallel to the circuit. Consequently, the reduced of the subcell D-2 will decrease the overall of the three-terminal cell; (III) on the other hand, as the thickness of the subcell D-1 is fixed, a thicker subcell D-2 absorbs more incident light, leading to the higher and efficiency.

4. Summary

We designed and simulated a new three-terminal a-Si solar cell. This structure improved the efficiency limitation that existed as a result of defects of a-Si solar cells. The efficiency of a 0.28 μm-thick thin-film three-terminal a-Si solar cell achieved 11.4%. The efficiency of the three-terminal a-Si solar cell could reach ~11.7% with the optimized thickness.

Acknowledgments

The authors are grateful to the National Center for High-Performance Computing for computer time and facilities (ISE TCAD). This work is supported by the National Science Council of Taiwan. under Contract no. 97-2218-E-259-006 and no. 98-2221-E-259-002-MY3.

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Copyright © 2011 Cheng-Hung Tai 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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