# To Enhance Performance of Light Soaking Process on ZnS/CuIn1-xGaxSe2 Solar Cell

Authors: Yu-Jen Hsiao; Chung-Hsin Lu; Te-Hua Fang
Journal: International Journal of Photoenergy
 (2013)

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## Abstract

The ZnS/CuInGaSe2 heterojunction solar cell fabricated on Mo coated glass is studied. The crystallinity of the CIGS absorber layer is prepared by coevaporated method and the ZnS buffer layer with a band gap of 3.21 eV. The MoS2 phase was also found in the CuInGaSe2/Mo system form HRTEM. The light soaking effect of photoactive film for 10 min results in an increase in F.F. from 55.8 to 64%, but series resistivity from 7.4 to 3.8 Ω. The efficiency of the devices improved from 8.12 to 9.50%.


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## Body

## 1. Introduction

Various photovoltaic (PV) devices have received a lot of attention as a renewable energy source [1]. These devices are made based on inorganic or organic materials, such as silicon-based thin film solar cells [2], multijunction solar cells [3], and dye-sensitized solar cells [4]. However, most of these devices suffer from either high cost or relatively low energy conversion efficiency. CuIn1-xGaxSe2 (CIGS)-based thin films have received considerable attention as one of the most promising materials for thin film solar cells due to their high absorption coefficient, the potential for low cost manufacturing, and high conversion efficiency for inorganic solar cell application, although Mo/CuInGaSe2 (CIGS) thin film solar cells have been extensively studied [5].A high efficiency CIGS is usually fabricated by a coevaporation method, but this is a complex process to scale up to large areas due to the problem of nonuniformity. Several low cost and promising alternatives to coevaporation suitable for large scale production, such as sputtering [6], electrodeposition [7], and screen printing [8], have been investigated. In particular, sputtering of CuInGa precursors followed by selenization appears to be a favored process for thin film deposition [9]. In this study, a three-stage co-evaporation deposition technology was adopted to grow CIGS photovoltaic/electronic films to realize efficient solar cells. To avoid the Cd-induced pollution to environment, the n-type ZnS buffer layer for forming CIGS PVs was introduced [10].In this paper, we report ZnS/CuIn1-xGaxSe2 heterojunction solar cells fabricated on Mo coated glass. The crystallinity of the CIGS and ZnS buffer layer were studied. The microstructure phase was investigated in the CuInGaSe2/Mo system by HRTEM. The light soaking and electrical properties of the fabricated p-CIGS/n-ZnS solar cells will also be discussed.


## 2. Experimental

The soda-lime glasses were carefully cleaned in isopropanol-acetone ultrasonic bath to remove electrostatic charges. An approximately 0.7μm thick Mo back contact was directly deposited by RF sputtering on glass substrate. CIGS absorber layers were deposited by evaporation of elemental Cu, In, Ga, and Se onto Mo by three-stage co-evaporation. During the 1st stage of the absorber growth the substrate temperature was kept at 400°C, while during the 2nd and 3rd stages the substrate temperature increased up to 600°C. The 100–300 nm thick ZnS buffer layer was deposited on CIGS film by chemical bath deposition at 80°C. The solar cells were finished by deposition of a ZnS buffer layer, RF sputtering of ZnO : Al front contacts (~400 nm thick), and electron beam evaporation of 1 μm thick Al contact grids for better current collection. No antireflection (AR) coating was applied.The phase identification was performed by X-ray powder diffraction (XRD, Rigaku Dmax-33). The surface microstructure was examined by scanning electron microscopy (SEM, Hitachi S4200). The morphology and microstructure were examined by transmission electron microscopy (HRTEM, HF-2000, Hitachi). The absorption spectra were obtained using an optical spectrometer (Hitachi, U-4100), and current-voltage measurements (Keithley 2410 SourceMeter) were obtained using a solar simulator (TELTEC) with an AM 1.5 filter under an irradiation intensity of 100 mW/cm2.


## 3. Results and Discussion

The CIGS quaternary alloy absorber layer coevaporated exhibits the characteristic peaks of chalcopyrite structure in X-ray diffraction (XRD) analysis, as shown in Figure1(a). XRD spectra also indicate that the CIGS film presents a strong (112) preferred orientation at 2θ = 26.68 corresponding to chalcopyrite phases. The other prominent peaks corresponded to the (220) and (312) directions. The full width at half maximum (FWHM) of the diffraction peak is rather small, which indicates that the film crystallinity is fairly good.(a) XRD spectra of CIGS film on Mo electrode. (b) XRD spectra of ZnS film synthesized using a chemical bath deposition method at various thicknesses.
(a)
(b)XRD patterns of ZnS with various deposition thicknesses are shown in Figure1(b). The possible chemical reactions for the synthesis of ZnS films are as follows:
(1)[Zn(H2O)5(OH)]++H+⟷Zn(OH)2+2H+(2)CH3CSNH2+H++2H2O⟷H2S+CH3COOH+NH4+(3)H2S⟷HS-+H+⟷S2-+H+(4)Zn2++S2-⟶ZnSDuring the reaction processes, sulfide ions are released slowly from CH3CSNH2 and react with zinc ions. It indicates that ZnS is produced by reaction of S2− and Zn2+ in (4). All of the peaks were identified to be those of the cubic ZnS phase (JCPDS card number 79-0043) [11]. The crystallinity of ZnS increased along with deposition thickness. When the thickness was increased from 100 to 300 nm, the peaks of (111), (220), and (311) were obviously shown.Figure2(a) has shown the UV-vis absorption spectra of 200 nm ZnS film on glass and estimated the band gap. For a direct band gap semiconductor, the absorbance in the vicinity of the onset due to the electronic transition is given by the following equation:
(5)α=C(hν-Eg)1/2hν,(a) Absorption spectra are as the function of photon energy for the 200 nm ZnS film. (b) Realized sample of ZnS film deposited on CIGS/Mo substrate.
(a)
(b)whereα is the absorption coefficient, C is the constant, hν is the photon energy, and Eg is the band gap. The visible light absorption edge of 200 nm ZnS film was at 386 nm. Extrapolation of the linear region gives a band gap of 3.21 eV. Therefore, the direct band gap energy obtained from our experiment is 3.21 eV. As known, hydrothermal process may transform some elemental S species to sulfur dioxides. It has defect states like S vacancies in the band gap of ZnS [12]. Therefore, the sample had lower band gap than ideal crystal structure of ZnS with 3.68 eV. It has shown actual sample of ZnS film before and after being deposited on CIGS/Mo substrate in Figure 2(b). The color of CIGS/Mo was gray on the surface, and then we can see brown color as ZnS film deposited on CIGS/Mo substrate. Therefore, we can determine ZnS film on CIGS by color variability.Figure3(a) shows the cross-sectional bright field TEM image of the Mo/CIGS/ZnS stacked layers. In contrast to the relatively large grains of the CIGS layer (0.2 to 0.7 μm), the ZnS layer consists of very small grains. Although the CIGS layer exhibits substantial surface roughness (~80 nm in average), the ZnS layer grown on top of CIGS has a uniform thickness (~200 nm) that was prepared for TEM by the focused ion beam (FIB). Each one of the layers constituting the Mo/CIGS/ZnS system was investigated in order to know the formation of defects as well as to get information regarding crystalline structure and grain size. On the other hand, two different regions are identified in the ZnS and CIGS/Mo films as is observed in the micrograph of Figures 3(b)-3(c). The crystalline ZnS films are identified by the high resolution lattice images. A representative HRTEM image enlarging a round part of the structure in Figure 3(b) is given. The interplanar distances of the crystal fringes are about 0.31 nm.Figure 3
(a) TEM cross-section images of ZnS/CIGS/Mo, (b) high-resolution TEM image of the cubic ZnS film, and (c) the interface of CIGS and Mo.The microstructure of the Mo/CuInGaSe2 interfaces was investigated in order to visualize defects and the formation of secondary phases as a result of possible chemical reactions occurring during the deposition of the stacked layers. Figure 3(c) shows a typical cross-sectional HRTEM image of the Mo/CIGS interface. The formation of a very thin layer (10–40 nm) of a new compound is observed around the Mo/CIGS interface. It seems that the new compound corresponds to the MoS2 phase due to the similarity with the CuInGaSe2/Mo system in which an interlayer of MoSe2 is usually formed [13]. This result makes sure that the metallic Mo thin layer is converted into MoS2 during the initial minutes of CIGS deposition. The MoS2 layer gives rise to a small conduction band offset with respect to the CIGS bulk material and a small Schottky barrier at the Mo back contact [14]. Both features are good for device performance, because the conduction band offset diminishes the back surface recombination, and then arrow Schottky barrier gives no substantial resistance to holes between CIGS and the metallic back contact. The EDS line profiles indicate that the CIGS film consists of Cu, In, Ga, and Se, as shown in Figure 4. In addition, the atomic concentrations of Cu = 23%, In = 21%, Ga = 10%, and Se = 46% are calculated from the EDS spectrum.Figure 4
EDX analysis of the CIGS film.Before light soaking the AZO/ZnS/CIGS heterojunction solar cell generally suffered from poor one-diode behaviour, a characteristic especially marked at low temperatures. The situation is considerably improved after light soaking with various times, under AM1.5G at 100 mW/cm2 illumination. The solar cell parameters of the cells used in photovoltaic measurements in Table 1. The time needed for the parameters to saturate under illumination is also shown. Before light soaking the problem with the cells was the low fill factor and high series resistivity. The fill factor increased significantly with light soaking for ZnS buffer layer, while Voc remains stable. In Figure 5(a), J-V curves obtained in the light soaked states for the lighting 5 and 10 min.Table 1
Photovoltaic performance of the AZO/ZnS/CIGS heterojunction solar cell with various light soaking times, under AM1.5G at 100 mW/cm2 illumination.
Lightsoaking
V
oc
(V)
J
sc (mA/cm2)
F.F. (%)
R
s (Ω)
R
sh (Ω)
η (%)
0 min
0.58
25.07
55.8
7.4
995
8.12
5 min
0.58
25.02
61.8
5.6
1023
8.97
10 min
0.60
24.88
64.0
3.8
1087
9.50(a)J-V characteristics of ZnS/CIGS heterojunction solar cell with various light soaking times and (b) the IPCE spectrum of CIGS solar cell with efficiency of 9.5%.
(a)
(b)The measurements reveal that lighting into the photoactive film results in an increase in F.F. from 55.8 to 64%, but series resistivity from 7.4 to 3.8 Ω. Theη value of the devices improved from 8.12 to 9.50%. The effect of F.F. value is attributed to the positive conduction band offsets (CBO) between the CIGS layer and the buffer layer, and it has been suggested that this barrier is lowered by illumination due to persistent photoconductivity (PPC) in the buffer layer [15]. In this work white light-induced metastable changes to the F.F. are only observed for cells with buffer layers having a lighting time 10 min. In addition, the quantum efficiencies are measured after light soaking in Figure 5(b). The EQE spectra are similar in shape, consistent with the almost unchanged short circuit current density.


## 4. Conclusions

In summary, the ZnS/CuInGaSe2 heterojunction solar cell with the light soaking process has been investigated. The crystallinity of the CIGS absorber layer is fairly good by coevaporated method. ZnS buffer layer with a band gap of 3.21 eV was deposited on CIGS/Mo sample. The MoS2 phase was found in the CuInGaSe2/Mo system form HRTEM. The light soaking effect of photoactive film for 10 min results in an increase in F.F. from 55.8 to 64%, but series resistivity from 7.4 to 3.8 Ω. The η value of the devices improved from 8.12 to 9.50%.



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*Source: 561948-2013-11-18.xml*