Open Access

Passivation ability of graphene oxide demonstrated by two-different-metal solar cells

  • Wen-Tzu Hsu1,
  • Zong-Sian Tsai1,
  • Liang-Chun Chen1,
  • Guan-Yu Chen1,
  • Chun-Chieh Lin2,
  • Mei-Hsin Chen1,
  • Jenn-Ming Song3 and
  • Chu-Hsuan Lin1Email author
Nanoscale Research Letters20149:696

Received: 27 June 2014

Accepted: 10 December 2014

Published: 23 December 2014


The study on graphene oxide (GO) grows rapidly in recent years. We find that graphene oxide could act as the passivation material in photovoltaic applications. Graphene oxide has been applied on Si two-different-metal solar cells. The suitable introduction of graphene oxide could result in obvious enhancement on the efficiency. The simple chemical process to deposit graphene oxide makes low thermal budget, large-area deposition, and fast production of surface passivation possible. The different procedures to incorporate graphene oxide in Si two-different-metal solar cells are compared, and 21% enhancement on the efficiency is possible with a suitable deposition method.


Passivation Solar cell Graphene oxide Two-different-metal Hummers method


Energy from solar cells has been thought as the possible alternative to the traditional fuel energy. In order to compete with the traditional energy, increase on the efficiency of solar cells in a cost-effective way is important. For a solar module with an efficiency of 20%, 1% improvement on efficiency can correspond to 5% reduction in cost. Surface structures[13] and passivation[47] can be utilized to improve the efficiency. Passivation of bare Si surfaces can be easily achieved with hydrogen termination, alkylation, and so on, but the effect may deteriorate in a certain time[8]. Passivation by dielectric films, such as SiO2, SiNx, and Al2O3 could overcome the stability issue. The high-quality SiO2 is common oxide for surface passivation of Si solar cells. Al2O3 prepared by atomic layer deposition is also used due to its promising ability of passivation for Si, especially for the p-type Si. Since various oxide materials have been used for passivation of solar cells, we would like to investigate the effect of graphene oxide (GO) as the passivation layer. GO is broadly studied after the developing of graphene in recent years[911]. The above mentioned oxide passivation films are almost demonstrated in chambers, and GO deposited in chemical solution may be a much simpler method. For the photovoltaic applications, GO has been adopted in organic solar cells as the hole transport layer[12]. We will apply GO to Si solar cells with the purpose of surface passivation. The different procedures to incorporate GO in Si two-different-metal solar cells are compared. To the best of our knowledge, GO has not been utilized on the applications of solar cell passivation. The chemical solution method makes the low thermal budget, large-area deposition, and fast production possible.


A two-different-metal structure for solar cells[13] was used in this study, because it could be fabricated easily in the laboratory and the passivation effect could be singly investigated on the side without electrodes. Figure 1 shows the schematic structure of the two-different-metal solar cell. The work functions of Au and Al are 5.1 and 4.18 eV, respectively, and hence, a built-in potential can be formed for photovoltaic application. In ref.[13], a thinned thermal SiO2 with high quality was inserted between the metals and Si. A critical high pressure H2O vapor heat treatment was also needed to obtain a satisfied interface. Since we were only interested in the effect of GO, the native oxide (SiO2) was kept instead of the high-quality thermal SiO2. We also found that if the top native oxide was removed, Au and Al might be easily shorted via the path of semiconductor. Hence, the native oxide was kept. Four kinds of cell structures (SiGb1, SiGb2, GbSi, and ConSi) were prepared and compared. The top sides of 1 to 30 Ω-cm p-type CZ Si substrates were evaporated by Al and Au in advance to prepare the sample ‘SiGb1’ and ‘SiGb2’. The difference between SiGb1 and SiGb2 only appeared on the procedures of GO deposition. Before the GO deposition, GO suspension should be prepared. First, graphite oxide was prepared by the modified Hummers method[14]. Subsequently, graphite oxide was added in the DI water and followed by two-step ultrasonication and centrifugation with a procedure similar to those in ref.[15, 16]. After the fist ultrasonication for 30 min, the solution was centrifuged at 4,000 r/min for 30 min. The supernatant was again ultrasonicated for 2 h followed by centrifugation at 10,000 r/min for 15 min. The ultrasonication was performed to exfoliate the GO sheets from graphite-oxide multilayer flakes. The GO sheets were hydrophilic due to their oxygen-containing groups, and the supernatant after centrifugation was dispersed with smaller and thinner flakes. The final supernatant was the GO suspension. The SiGb1 sample was prepared via the dip coating method. The topside-down Si substrate was immersed in the GO suspension for 40 min to coat GO sheets on the side without electrodes (rear side), and it was taken out to dry naturally to obtain the SiGb1 sample. To fabricate the SiGb2 sample, the GO suspension was only dropped on the rear surface of the Si substrate instead of the immersion of the entire substrate. This SiGb2 sample was dried at 70°C on the hot plate. Then, the SiGb2 sample was obtained. In ref.[15], the Si substrates with hydrophilic treatment in the Standard Cleaning 1 (SC1) solution with NH4OH:H2O2:H2O = 1:2:8 before GO deposition could own a dense coverage of GO. We would like to prepare a similar sample with SC1 treatment. However, we found that the electrodes of the cells would exfoliate when immersing in the SC1 solution. Hence, we prepared a sample named as ‘GbSi’, where the Si substrate was SC1 (hydrophilicly) treated in advance. Dip coating and drying of GO suspension were then performed, and electrodes were evaporated finally. A similar two-metal structure without the GO deposition, named as ‘ConSi’, was also fabricated for comparison.
Figure 1

The schematic structure of the Si two-different-metal solar cell. The work functions of Au and Al are 5.1 and 4.18 eV, respectively, and hence, a built-in potential can be formed.

Results and discussion

The current versus voltage (IV) characteristics of the samples with AM 1.5 G illumination from the top side (the side with electrodes) are shown in Figure 2. When light is irradiated from the top surface, the short-circuit current (ISC) of the SiGb1, SiGb2, ConSi, and GbSi cells are 1.930, 1.703, 1.603, and 1.563 mA, respectively. The open-circuit voltage (VOC) are 0.423, 0.409, 0.408, and 0.376 V, respectively. Both SiGb1 and SiGb2 show better performance as compared with the reference ConSi cell. It proves that GO indeed owns the ability to passivate the Si solar cells. It should be mentioned that in the current stage, the solar cell is not optimized on the efficiency, and hence, the efficiency is not good enough. Hence, we only focus on ISC and VOC in order to indicate the influence contributed by GO. Because the Au and Al should be evaporated by shadow masks in different runs, the alignment between runs limits the pattern. The pattern could not be optimized just considering carrier generation and collection. The device area is 0.72 cm2, but the effective area without electrode shielding is only 0.19 cm2. Hence, the best GO (SiGb1) and control cells (ConSi) can only own efficiencies of 0.63% and 0.52%, respectively. Although the absolute value of efficiency is low due to the un-optimized cell structure, the results indicate that the GO introduction can contribute up to 21% enhancement on the efficiency. The dark current density versus voltage characteristics of SiGb1 and ConSi are also shown in Figure 3. The smaller dark reverse (negative bias) current density of the SiGb1 cell contributes to its higher VOC as compared to ConSi[17].
Figure 2

The current versus voltage characteristics with AM 1.5 G illumination from the top side. The device area is 0.72 cm2. The inset shows that the deposited SiNx film results in a poor performance.

Figure 3

The dark current density versus voltage characteristics of SiG b 1 and ConSi. The smaller dark reverse (negative bias) current density of the SiGb1 cell contributes to its higher VOC as compared to ConSi.

The other GO sample, GbSi, shows a worse performance than the ConSi. In order to find the reason for degradation of GbSi, the atomic force microscope (AFM) images of samples with GO deposition were measured (Figure 4). The AFM images show that the SC1 treatment resulted in a much thick GO film on the rear side of Si of GbSi (Figure 4c) as compared with those of SiGb1 (Figure 4a) and SiGb2 (Figure 4b). The highly hydrophilic surface of GbSi may also attract GO flakes on the top side (sides with electrodes). The GO flakes between Si and electrodes would prevent the current conduction, which results in the poor performance of GbSi as compared to the ConSi.
Figure 4

The AFM images of (a) SiG b 1, (b) SiG b 2, and (c) G b Si samples. For the sample of SiGb1, the deposited GO film was approximately 20 nm in thickness. On the other hand, the GO film on GbSi is much thicker due to the extra SC1 treatment before GO deposition.

The passivation effect of GO is supposed due to the field effect passivation contributed by the negative fixed charge in GO as verified in ref.[15]. In ref.[15], the capacitance verse voltage relation of GO and control metal-insulator-semiconductor (MIS) capacitors were compared. The curves of MIS capacitors with GO coated shifted to the positive-bias direction, and it meant that extra negative charge existed in GO. Such a dielectric GO film with negative fixed charge could be used to passivate solar cells, especially for the p-side. For our two-different-metal solar cells, GO can be coated on the rear side of the p-type Si substrate. Without GO being coated, many of the photo-generated electron-hole pairs may easily recombine at the rear surface due to the termination of the periodic Si structure. With GO coated, minority carriers (electrons) can be repelled from the surface. Since recombination should only occur between an electron and a hole, the repulsion of electron from the surface could contribute to the decrease of recombination. More electrons can be collected by the Al electrode successfully, and hence, more holes can be collected by the Au electrode. That is why SiGb1 and SiGb2 show the better performance as compared with the ConSi.

Silicon nitride (SiNx) is a common passivation film for solar cells. We have also prepared a two-different-metal solar cell with SiNx on the rear side for comparison. First, we demonstrated another control two-different-metal solar cell, ConSi2, and its IV characteristic under AM 1.5 G illumination was obtained as shown in the inset of Figure 2. Then, the native oxide on the rear side of ConSi2 was removed by buffered oxide etch (BOE). SiNx was subsequently deposited on the rear side by the sputter. Its IV characteristic is also shown in the inset of Figure 2 as the curve of ‘ConSi2 with SiNx’. It can be found that the performance of ‘ConSi2 with SiNx’ is even worse than ConSi2. One reason for the degradation may be due to the un-optimized facility for passivation. The sputter SiNx might have poor quality as compared with the commercial PECVD SiNx. The other reason is that SiNx with positive fixed charge is more suitable for passivation of n-Si substrates instead of p-Si substrates in our case[18].

Because the best GO cell, SiGb1, has been immersed in the GO suspension for 40 min, it may be suspected that the performance enhancement is due to the more oxidation in water (in GO suspension) but not GO deposition. We prepared two extra control samples. One was immersed in DI water, and the other was rear-side down floating on the water surface of GO suspension to have the similar immersion condition but avoid GO deposition. These two control samples after immersion did not show better cell performance than the results before immersion (not shown here), indicating that the improvement was indeed only due to the GO passivation on the surface.

In ref.[13], the light illumination from the rear surface results in a larger short-circuit current density (Jsc) than that from the top surface, which is due to the avoidance of electrode shading. However, the ISC of our control cell (ConSi) with rear illumination (Figure 5) is smaller than top illumination (Figure 2), since the rear side of our control cell is not coated by the 100-nm-thick oxide (performed in ref.[13]). Furthermore, the ISC of all GO samples is even smaller than that of ConSi. It is suspected that some of incident light is absorbed by GO. The transmittance spectrum of GO on glass has been measured by Fourier transform infrared spectroscopy (FTIR) (Figure 6). In Figure 6, with an incident wavelength of 550 nm, the transmittance of GO on glass is only 87%. The deposition of GO reduces the amount of light entering the Si, and hence the ISC of the GO samples is smaller than that of the control sample for the rear-side illumination case. Although ISC of SiGb1 and SiGb2 can not be superior than ConSi, VOC of both samples can still be superior than ConSi. The lower recombination contributed by GO corresponds to a smaller reverse current, which results in a larger VOC as mentioned above.
Figure 5

Current versus voltage characteristics with AM 1.5 G illumination from the rear side. With rear illumination, ISC of the SiGb1, SiGb2, ConSi, and GbSi cells are 1.000, 0.999, 1.040, and 1.000 mA, and VOC are 0.400, 0.383, 0.374, and 0.370 V, respectively. GO samples own smaller JSC as compared to ConSi because partial input light will be absorbed by GO on the rear side.

Figure 6

The transmittance of the glass with a GO film. The deposition condition of this GO film on glass is similar to that of SiGb1. The reference background in this FTIR measurement is air instead of glass to avoid the large fluctuation after dividing by background.


GO is first-time proven to have the ability to enhance the performance of a solar cell by surface passivation due to its negative fixed charge. GO provides the potential on low-cost and large-area passivation. In the current stage, the simple two-different-metal structure is adopted as the beginning. Further optimization on deposition conditions and light transmission is deserved. More efforts should be made to incorporate the benefit of GO in commercial Si pn solar cells.



This work is supported by National Science Council of R.O.C. under contract no. NSC 101-2221-E-259-023-MY3.

Authors’ Affiliations

Department of Opto-Electronic Engineering, National Dong Hwa University
Department of Electrical Engineering, National Dong Hwa University
Department of Materials Science and Engineering, National Chung Hsing University


  1. Cacciato A, Duerinckx F, Baert K, Moors M, Caremans T, Leys G, Keersmaecker K, De Szlufcik J: Investigating manufacturing options for industrial PERL-type Si solar cells. Sol Energy Mater Sol Cells 2013, 113: 153–159.View ArticleGoogle Scholar
  2. Chen TG, Huang BY, Chen EC, Yu P, Meng HF: Micro-textured conductive polymer/silicon heterojunction photovoltaic devices with high efficiency. Appl Phys Lett 2012, 101: 033301. 10.1063/1.4734240View ArticleGoogle Scholar
  3. Ha JM, Yoo SH, Cho JH, Cho YH, Cho SO: Enhancement of antireflection property of silicon using nanostructured surface combined with a polymer deposition. Nanoscale Res Lett 2014, 9: 9. 10.1186/1556-276X-9-9View ArticleGoogle Scholar
  4. Sameshima T, Kogure K, Hasumi M: High-quality surface passivation of silicon using native oxide and silicon nitride layers. Appl Phys Lett 2012, 101: 021601. 10.1063/1.4733336View ArticleGoogle Scholar
  5. Chen J, Cornagliotti E, Loozen X, Simoen E, Vanhellemont J, Lauwaert J, Vrielinck H, Poortmans J: Impact of firing on surface passivation of p-Si by SiO2/Al and SiO2/SiNx/Al stacks. J Appl Phys 2011, 110: 126101. 10.1063/1.3669405View ArticleGoogle Scholar
  6. Schmidt J, Merkle A, Brendel R, Hoex B, van de Sanden MCM, Kessels WMM: Surface passivation of high-efficiency silicon solar cells by atomic-layer-deposited Al2O3. Prog Photovolt 2008, 16: 461–466. 10.1002/pip.823View ArticleGoogle Scholar
  7. Zhao Y, Zhou C, Zhang X, Zhang P, Dou Y, Wang W, Cao X, Wang B, Tang Y, Zhou S: Passivation mechanism of thermal atomic layer-deposited Al2O3 films on silicon at different annealing temperatures. Nanoscale Res Lett 2013, 8: 114. 10.1186/1556-276X-8-114View ArticleGoogle Scholar
  8. Royea WJ, Juang A, Lewis NS: Preparation of air-stable, low recombination velocity Si(111) surfaces through alkyl termination. Appl Phys Lett 2000, 77: 1988–1990. 10.1063/1.1312203View ArticleGoogle Scholar
  9. Joshi RK, Carbone P, Wang FC, Kravets VG, Su Y, Grigorieva IV, Wu HA: Precise and ultrafast molecular sieving through graphene oxide membranes. Science 2014, 343: 752–754. 10.1126/science.1245711View ArticleGoogle Scholar
  10. Wang W, Li Z, Duan J, Wang C, Fang Y, Yang XD: In vitro enhancement of dendritic cell-mediated anti-glioma immune response by graphene oxide. Nanoscale Res Lett 2014, 9: 311. 10.1186/1556-276X-9-311View ArticleGoogle Scholar
  11. Liu J, Kim GH, Xue Y, Kim JY, Baek JB, Durstock M: Graphene oxide nanoribbon as hole extraction layer to enhance efficiency and stability of polymer solar cells. Adv Mater 2014, 26: 786–790. 10.1002/adma.201302987View ArticleGoogle Scholar
  12. Li SS, Tu KH, Lin CC, Chen CW, Chhowalla M: Solution-processable graphene oxide as an efficient hole transport layer in polymer solar cells. ACS Nano 2010, 4: 3169–3174. 10.1021/nn100551jView ArticleGoogle Scholar
  13. Sameshima T, Kogure K, Hasumi M: Crystalline silicon solar cells with two different metals. Jpn J Appl Phys 2010, 49: 110205. 10.1143/JJAP.49.110205View ArticleGoogle Scholar
  14. Lin CH, Yeh WT, Chan CH, Lin CC: Influence of graphene oxide on metal-insulator-semiconductor tunneling diodes. Nanoscale Res Lett 2012, 7: 343. 10.1186/1556-276X-7-343View ArticleGoogle Scholar
  15. Lin CH, Yeh WT, Chen MH: Metal-insulator-semiconductor photodetectors with different coverage ratios of graphene oxide. IEEE J Sel Top Quantum Electron 2014, 20: 3800105.Google Scholar
  16. Wang X, Zhi L, Müllen K: Transparent, conductive graphene electrodes for dye-sensitized solar cells. Nano Lett 2008, 8: 323–327. 10.1021/nl072838rView ArticleGoogle Scholar
  17. Singh P, Ravindra NM: Temperature dependence of solar cell performance-an analysis. Sol Energy Mater Sol Cells 2012, 101: 36–45.View ArticleGoogle Scholar
  18. Hoex B, Schmidt J, Pohl P, van de Sanden MCM, Kessels WMM: Silicon surface passivation by atomic layer deposited Al2O3. J Appl Phys 2008, 104: 044903. 10.1063/1.2963707View ArticleGoogle Scholar


© Hsu et al.; licensee Springer. 2014

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