International Journal of Photoenergy

Volume 2014 (2014), Article ID 762576, 5 pages

http://dx.doi.org/10.1155/2014/762576

Research Article

Characterization of Cu1.4Te Thin Films for CdTe Solar Cells

Guangcan Luo, Bin Lv, Wei Li, Lianghuan Feng, Jingquan Zhang, Lili Wu, and Guanggen Zeng

College of Materials Science and Engineering, Sichuan University, Chengdu 610064, China

Received 17 February 2014; Accepted 28 April 2014; Published 15 May 2014

Academic Editor: Prakash Basnyat

Copyright © 2014 Guangcan Luo 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.

The copper telluride thin films were prepared by a coevaporation technique. The single-phase Cu1.4Te thin films could be obtained after annealing, and annealing temperature higher than 220°C could induce the presence of cuprous telluride coexisting phase. Cu1.4Te thin films also demonstrate the high carrier concentration and high reflectance for potential photovoltaic applications from the UV-visible-IR transmittance and reflectance spectra, and Hall measurements. With contacts such as Cu1.4Te and Cu1.4Te/CuTe, cell efficiencies comparable to those with conventional back contacts have been achieved. Temperature cycle tests show that the Cu1.4Te contact buffer has also improved cell stability.

1. Introduction

Copper chalcogenides have attracted much interest because of their potential applications in thermoelectric devices [1] and in heterojunction structures [2–7]. Cusano [3] prepared a CdTe solar cell with an efficiency of 7.5% in which cuprous telluride (Cu₂Te) was used as a p-type partner to the n-type CdTe semiconductor. To further improve device performance of CdTe solar cells, Cu₂Te is commonly used as a p-type back contact layer to facilitate low resistance contact formation [4, 5]. However, due to the fast diffusivity of Cu in CdTe and the apparent instability of Cu₂Te (Cu₂Te→CuTe + Cu, Cu₂Te→2Cu + αTe + 1/2()Te₂ [8, 9]), copper is suspected to be responsible for changes in cell performance and stability with exposure to light [10–12]. Since this particular element plays a key role in cell performance and characteristics, it is important to minimize the Cu supply while maintaining the ohmic characteristics of p⁺ CdTe contact. Thus, an extensive investigation of the properties of copper tellurides (CuxTe) and stability of CdTe-based solar cells with CuxTe has been carried out [13]. It has been found that CuxTe shows bistability with energy minimum at and [13]. These results using first-principles calculations are consistent with experimental observations, which find stable CuxTe structures at two different Cu concentrations (i.e., and [6, 7]). The calculated minimum energy concentrations are slightly smaller than experimental observations due to the fact that strain and temperature effects are not included in the calculation. Therefore, in our work, CuxTe thin films at low x () were prepared by vacuum coevaporation. The properties of CuxTe thin films at low x were studied and performance of CdTe solar cells with CuxTe was investigated and also monitored with the temperature cycle test.

2. Experimental Details

Cu1.4Te thin films were deposited on a simultaneous evaporation system DM-400 to a thickness of ~200 nm at room temperature. Cu foil (99.999% purity) and Te powder (99.999% purity) were evaporated on substrates from two independent sources, respectively. The deposition rate and the thickness of thin films were monitored by two-thickness monitors (LHC-2, Huazhao Industrial Ltd., China). After deposition, a posttreatment was performed at different temperatures in N₂ ambient. X-ray diffraction (XRD) (DX-2600, Dandong Fangyuan Instrumental Ltd., China) measurements were used to study the copper telluride structure. The transmittance and reflectance spectra were used to investigate the optical properties of materials. The four-probe Van der Pauw method was used to carry out the Hall measurements to determine the Hall coefficient, mobility, and carrier concentration.

Solar cells were fabricated in a superstrate configuration typical of CdTe devices, that is, glass/TCO/CdS/CdTe/back contact. CdS thin films were deposited by a chemical bath deposition technique to a thickness of 180 nm onto the glass substrate coated with SnO₂:F. CdTe thin films were subsequently prepared in argon and oxygen ambient by close-spaced sublimation to a thickness of ~5 μm. Following the heat treatment of the samples in CdCl₂, the CdTe surface was etched in a bromine/methanol solution (0.05% vol.). The back contact, Cu1.4Te (~100 nm), was deposited on the etched CdTe surface by coevaporation. And then samples were treated in a pure N₂ ambient in the 180°C~220°C range. Finally, Ni thin films (~300 nm) prepared by electron beam evaporation were used as a back electrode to complete the back contacts processing. The photovoltaic devices were characterized using dark J-V measurement (4155C, Agilent, USA) and light J-V measurement (XJCM-9, Gsolar, China) under simulated AM1.5 illumination (100 mW/cm²). The device stability was performed using the high- and low-temperature cycle tests. As shown in Figure 1 one cycle was the process of the cycling through two temperature extremes (i.e., 85°C and −40°C).

Figure 1: The high- and low-temperature cycle testing curve.

3. Results and Discussion

3.1. Structural, Optical, and Electronic Properties of Cu1.4Te Thin Films

Copper telluride thin films were deposited by coevaporation at room temperature on glass substrates as shown in Figure 2. The thin films as-deposited were an amorphous structure. There are no changes in the phase for copper telluride thin films with annealing temperature up to 170°C. Then the thin films were annealed at 180°C in N₂ ambient. Copper telluride thin films annealed had some diffraction peaks. The peaks at about 2θ of 11.393°, 14.461°, 23.516°, 26.586°, 26.667°, 29.159°, 44.415°, 55.078°, and 60.501° correspond to the (021), (002), (051), (052), (004), (006), (204), and (176) planes of Cu1.4Te, respectively. The results also indicate that the Cu1.4Te thin films are single-phase hexagonal structure with random orientations when annealed at a higher temperature, that is, 200°C. Figure 2 shows XRD pattern of Cu1.4Te thin films annealed at 220°C. The intensity of these diffraction peaks for the thin films increased with annealing temperature. And there are remarkable differences among these two samples annealed at 200°C and 220°C. The peak at 2θ of 12.9°, corresponding to the lattice spacing of 6.8487 Å, was indexed as the 1st order diffraction of the cupric telluride (CuTe). So, the peak positions of the (002), (003), and (004) planes at 2θ of 25.8°, 40°, and 52.8° were the 2nd, 3rd, and 4th order diffraction of CuTe. The presence of other X-ray diffraction peaks associated with a CuTe phase indicated that the coexisting phase had occurred. It is obvious that annealing to 220°C results in the formation of coexisting phase for copper telluride thin films, which may have a strong influence on the stability of the CdTe-based solar cells. Therefore, the devices for this work were postannealed at 180°C~220°C, whose results will be discussed in Section 3.2.

(a)

(b)

(c)

(d)

Figure 2: XRD patterns of copper telluride thin films as deposited and annealed at different temperatures.

The optical properties of Cu1.4Te thin films with a single-phase hexagonal structure were studied using the UV-Visible-IR transmittance and reflectance spectra as shown in Figure 3. The transmittance of no more than 30% for Cu1.4Te thin films in the range of 300~900 nm was observed. While the reflectance for the thin films increased up to ~50% in the range from 500 to 900 nm, which may reflect the photons in this range to p-n junction. It can be inferred that the thickness of the absorption layer, CdTe, can be reduced in the CdTe solar cells due to the incorporation of the thin films, Cu1.4Te, as the back contact. From the optical properties of Cu1.4Te thin films we suggest that it may be a kind of good photovoltaic materials in CdS/CdTe heterojunction solar cells.

Figure 3: Transmittance and reflectance spectra for Cu1.4Te thin films.

The electronic properties of single-phase Cu1.4Te thin films from the Hall measurements were also investigated. Table 1 shows the parameters for Cu1.4Te thin films such as the mobility, Hall coefficient, and carrier concentration. The results show that Cu1.4Te thin films were p-type semiconductor compounds and had high carrier concentration, ~10²¹ cm⁻³. The high carrier concentration means high conductivity which can reduce series resistance of the solar cells with a Cu1.4Te layer and thus improve remarkably the device performance. Table 1 also shows that the mobility of Cu1.4Te thin films is very low. The carrier mobility has the following relation:

where is the elementary charge, is the relaxation time, and is the effective mass. Because the carrier effective mass did not alter much, it is deduced that the increase of the mobility is due to the decrease of the relaxation time, which inverses to the scattering probability. Therefore, further improvement in the thin films, such as less defects, small strain, and large grain sizes, for practical use can be made.

Table 1: Parameters for Cu1.4Te thin films.

Sample
Mobility

(cm²/V*S)
Hall coefficient

(cm³/Cb)
Carrier concentration

(cm⁻³)

Cu1.4Te
13.82
0.0042
1.48 × 10²¹

3.2. CdTe Solar Cells with Cu1.4Te Thin Films

In this work, the device configuration consisted of a glass/SnO₂/CdS/CdTe/back contact/Ni structure, where back contact was Cu1.4Te thin films. After chemical etching, the Cu1.4Te thin films were deposited on the CdTe thin films and annealed in N₂ ambient. Figure 4 shows the XRD pattern of CdTe solar cells with a Cu1.4Te layer annealed at 200°C before metallization. Besides the diffraction peaks of CdTe, the XRD pattern demonstrates the other phase with weak diffraction intensity, which can be indexed to (051) planes of Cu1.4Te thin films.

Figure 4: XRD pattern of Cu1.4Te thin films deposited on the CdTe thin films.

To investigate the effect of Cu1.4Te thin films on back contact formation and device performance, device characterization was performed on CdTe devices. Table 2 shows the device parameters for CdTe solar cells with or without Cu1.4Te thin films annealed at different temperatures in N₂ ambient. One can see that CdTe solar cells made with a Cu1.4Te layer have better performance than those without Cu1.4Te back-contact. that is, the short circuit current (), open circuit voltage (), fill factor (FF) and conversion efficiency () increased for CdTe solar cells made with a Cu1.4Te layer. Annealing at high temperatures is commonly used in the back contact formation process for the diffusion and dopant activation [14]. In this work, higher was obtained when the cells were annealed at a higher temperature. This may be attributed to the increase of the acceptors. It can be seen that the device performance of CdTe solar cells with single-phase Cu1.4Te thin films annealed at 200°C is superior to that of the solar cells with coexisting phase copper telluride thin films at 220°C. We suggest that the single-phase Cu1.4Te thin films annealed at 200°C are more suitable for forming p-type back contacts between CdTe and the electrodes than coexisting phase thin films.

Table 2: Device parameters for CdTe solar cells with or without Cu1.4Te thin films.

(°C)
(mV)
(mA/cm2 )
(%)
FF (%)
Area (cm²)

nbc*
667
20.5
7.6
55
0.0707

180
721
22.7
9.7
57
0.19625

200
736
23.6
11.6
67
0.0707

220
788
21.0
9.5
57
0.19625

nbc denotes the cells without back contacts.

Dark J-V characteristic of solar cells (Figure 5) can be expressed by Shockley diode equation:

where stands for the diode current, denotes the dark saturation current, is the diode ideality factor. From the dark J-V characteristic curve (Figure 5), one can obtain a dark saturation current  mA/cm², and a diode quality factor , which is consistent with the results reported by Wu et al. [6], for CdTe solar cells with a single-phase Cu1.4Te layer annealed at 200°C. The illuminated J-V curve (see also Figure 5) compared to the dark J-V curve shows that the crossover is eliminated effectively due to the incorporation of the Cu1.4Te back contact.

Figure 5: Dark and light J-V curves for a CdS/CdTe/Cu1.4Te solar cell.

The stability of the solar cells with Cu1.4Te back contacts was evaluated with the temperature cycle tests. Table 3 shows the evolution of the photovoltaic parameters for the CdTe solar cells with Cu1·4Te. Under this environmental stress condition, some parameters of the device have quite random values as a function of stress time, which is similar to other environmental stress tests [12]. This may be evidence of the existence of traps within the absorber CdTe layers. The CdTe cell without Cu1.4Te degraded rapidly in cell efficiency from 8.33% to zero after 90 days and 9 cycles, whereas the CdTe cell with Cu1.4Te showed much improved stability with efficiency loss from 11.75% to 7.58% even after 420 days and 42 cycles. The degradation may be attributed in part to the unencapsulated cells in the laboratory and the back electrodes with exposure to moist air.

Table 3: Evolution of device parameters for CdTe solar cells with the temperature cycling.

Day and cycle
nbc
Cu1.4Te

(mV)
FF (%)
(mA/cm²)
(%)
(mV)
FF (%)
(mA/cm²)
(%)

Initial
695
55.9
21.45
8.33
732
67.4
23.81
11.75

30d3c*
676
46.4
19.33
6.74
709
58.4
22.95
9.50

90d9c
495
—
17.81
—
712
58.2
23.07
9.56

180d12c

708
57.0
22.56
9.10

420d42c

707
50.5
21.24
7.58

30d3c denotes 3 cycles after 30 days in the period of testing.

4. Conclusions

Copper telluride thin films were prepared by using the vacuum coevaporation method. At low temperature, the copper telluride thin films were an amorphous structure. In the temperatures ranging between 180 and 220°C, the copper telluride thin films indicate the form of the single-phase Cu1.4Te structure, whereas with annealing temperature higher than 220°C, the coexisting phase for the thin films occurs. With a Cu1.4Te as a back contact layer, efficient and stable CdTe solar cells can be obtained.

Conflict of Interests

The authors declare that there is no conflict of interests regarding the publication of this paper.

Acknowledgments

This work was supported by the National Basic Research Program of China (Grant no. 2011CBA007008), National Natural Science Foundation of China (Grant no. 61076058), and the Science and Technology Program of Sichuan Province, China (Grant no. 13ZC2185).

References

V. V. Gorbatchev, Semiconducting AI₂BVI compounds, Metallurgia, Moscow, Russia, 1980.

W. S. Chen, J. M. Stewart, and R. A. Mickelsen, “Polycrystalline thin-film Cu2-xSe/CdS solar cell,” Applied Physics Letters, vol. 46, no. 11, pp. 1095–1097, 1985.

D. A. Cusano, “CdTe solar cells and photovoltaic heterojunctions in II-VI compounds,” Solid State Electronics, vol. 6, no. 3, pp. 217–218, 1963.

B. Lv, X. Di, W. Li et al., “Preparation of Cu₂Te thin films and back-contact formation of CdTe solar cells,” Japanese Journal of Applied Physics, vol. 48, no. 8, pp. 0855011–0855014, 2009.

J. H. Yun, K. H. Kim, D. Y. Lee, and B. T. Ahn, “Back contact formation using Cu₂Te as a Cu-doping source and as an electrode in CdTe solar cells,” Solar Energy Materials and Solar Cells, vol. 75, no. 1-2, pp. 203–210, 2003.

X. Wu, J. Zhou, A. Duda et al., “Phase control of CuxTe film and its effects on CdS/CdTe solar cell,” Thin Solid Films, vol. 515, no. 15, pp. 5798–5803, 2007.

G. Lorenz and C. Wagner, “Investigations on cuprous selenide and copper tellurides,” The Journal of Chemical Physics, vol. 26, no. 6, pp. 1607–1608, 1957.

G. Teeter, “Cu₂Te synthesis and in-vacuum thermal decomposition: chemical-kinetics analysis and comparison to equilibrium vapor-pressure measurements,” Thin Solid Films, vol. 515, no. 20-21, pp. 7886–7891, 2007.

B. Brunetti, V. Piacente, P. Vassallo, and A. R. Villani, “A torsion-effusion study on the sublimation of Cu₂Te,” Materials Chemistry and Physics, vol. 70, no. 3, pp. 263–267, 2001.

P. R. Kharangarh, D. Misra, G. E. Georgiou, and K. K. Chin, “Characterization of space charge layer deep defects in n+-CdS/p-CdTe solar cells by temperature dependent capacitance spectroscopy,” Journal of Applied Physics, vol. 113, no. 14, Article ID 144504, pp. 1–6, 2013.

P. Kharangarh, D. Misra, G. E. Georgiou, and K. K. Chin, “Evaluation of Cu back contact related deep defects in CdTe solar cells,” ECS Journal of Solid State Science and Technology, vol. 1, no. 5, pp. Q110–Q113, 2012.

D. L. Bätzner, R. Wendt, A. Romeo, H. Zogg, and A. N. Tiwari, “Study of the back contacts on CdTe/CdS solar cells,” Thin Solid Films, vol. 361-362, pp. 463–467, 2000.

J. L. F. da Silva, S.-H. Wei, J. Zhou, and X. Wu, “Stability and electronic structures of CuxTe,” Applied Physics Letters, vol. 91, no. 9, Article ID 091902, 2007.

B. Biglari, M. Samimi, M. Hage-Ali, J. M. Koebel, and P. Siffert, “Effects of copper in high resistivity cadmium telluride,” Journal of Crystal Growth, vol. 89, no. 4, pp. 428–434, 1988.