共查询到20条相似文献,搜索用时 11 毫秒
1.
Takayuki Watanabe Hidenobu Nakazawa Masahiro Matsui Hiroki Ohbo Tokio Nakada 《Solar Energy Materials & Solar Cells》1997,49(1-4)
The controlled incorporation of sodium into the absorber layer of CuInS2 solar cells improved cell performance remarkably. Without toxic KCN treatment, conversion efficiencies of over 6% were achieved by sulfurization of sodium-containing precursors. We also investigated the characteristics of the sodium-incorporated CuInS2 films by intentional addition and diffusion from a soda-lime glass. The ternary compound semiconductor of NaInS2 was found to form mainly on the surface of each of the CuInS2 films. 相似文献
2.
A. Amara W. Rezaiki A. Ferdi A. Hendaoui A. Drici M. Guerioune J.C. Bernde M. Morsli 《Solar Energy Materials & Solar Cells》2007,91(20):1916-1921
Single crystals CuInS2 were grown by iodine vapour transport method, whereas polycrystalline thin films were obtained by coevaporation technique from three sources. The temperature dependence of the hole mobility in valence band is analysed by taking into account contributions from several scattering mechanisms of the charge carriers. To account for the temperature dependant conductivity of polycrystalline CuInS2 thin films, grainboundary conduction process was suggested. In the low temperature region, we interpret the data in terms of the Mott law and the analysis is very consistent with the variable range hopping. However, thermionic emission is predominant at high temperatures. Photoluminescence measurements have been performed on CuInS2 crystals and the analysis has revealed that the emission is mainly due to free-to-bound and donor–acceptor pair transitions. The band gap of that compound is derived from the excitonic emission line at 1.53 eV. 相似文献
3.
Juan Manuel Peza-Tapia Mauricio Ortega-López 《Solar Energy Materials & Solar Cells》2009,93(5):544-548
The specific contact resistivity (ρC) for aluminum (Al), silver (Ag) and indium (In) metallic contacts on CuInS2 thin films was determined from I-V measurements, with the purpose of having the most appropriate ohmic contact for TCO/CdS/CuInS2 solar cells; ρC was measured using the transmission line method (TLM) for the metallic contacts evaporated on CuInS2 thin films deposited by spray pyrolysis with ratios x=[Cu]/[In]=1.0, 1.1, 1.3 and 1.5 in the spray solution. The results show that In contacts have the lowest ρC values for CuInS2 samples grown with x=1.5. The minimum ρC was 0.26 Ω cm2 for the In contacts. This value, although not very low, will allow the fabrication of CuInS2 solar cells with a small series resistance. 相似文献
4.
Emma Cárdenas E. Perez-Tijerina T.K. Das Roy B. Krishnan 《Solar Energy Materials & Solar Cells》2009,93(1):33-36
We report the modification of electrical properties of chemical-bath-deposited antimony sulphide (Sb2S3) thin films by thermal diffusion of carbon. Sb2S3 thin films were obtained from a chemical bath containing SbCl3 and Na2S2O3 salts at room temperature (27 °C) on glass substrates. A carbon thin film was deposited on Sb2S3 film by arc vacuum evaporation and the Sb2S3-C layer was subjected to heating at 300 °C in nitrogen atmosphere or in low vacuum for 30 min. The value of resistivity of Sb2S3 thin films was substantially reduced from 108 Ω cm for undoped condition to 102 Ω cm for doped thin films. The doped films, Sb2S3:C, retained the orthogonal stibnite structure and the optical band gap energy in comparison with that of undoped Sb2S3 thin films. By varying the carbon content (wt%) the electrical resistivity of Sb2S3 can be controlled in order to make it suitable for various opto-electronic applications. 相似文献
5.
Rohana Garuthara Ruwan Wijesundara Withana Siripala 《Solar Energy Materials & Solar Cells》2003,79(3):331-338
Potentiostatic electrodeposition and sulfurization techniques were used to prepare polycrystalline CuInS2 thin films. X-ray diffraction and photoresponse measurements in a photoelectrochemical cell (PEC) revealed that photoactive polycrystalline CuInS2 films can be deposited on Ti substrate. Photoluminescence (PL) spectroscopy was used to investigate the prepared thin films and optically characterize them. PL spectra revealed the defect structure of the samples with an acceptor energy level at 109 meV above the valance band and a donor energy level at 71 meV below the conduction band. The CuInS2 thin films prepared in this investigation are observed to be In-rich material with n-type electrical conductivity. 相似文献
6.
A. Neisser I. Hengel R. Klenk Th. W. Matthes J. lvarez-García A. Prez-Rodríguez A. Romano-Rodríguez M. -Ch. Lux-Steiner 《Solar Energy Materials & Solar Cells》2001,67(1-4)
Thin film CuInS2:Ga solar cell absorber films were prepared by sequential evaporation of Cu–In–Ga precursors and sulfurization in sulfur vapor. The depth distribution of Ga was found to be highly inhomogeneous caused by CuGaS2 phase segregation at the back contact. Depending on overall Ga content and sulfurization temperature a quaternary CuGaxIn1−xS2 compound formed exhibiting a shift in absorber lattice constant and band gap. Micro Raman measurements showed that crystal quality was also affected by Ga. Open-circuit voltages well above 800 mV were achieved while sustaining high fill factors of 71%. 相似文献
7.
X.H. Xu F. Wang J.J. Liu K.C. ParkM. Fujishige 《Solar Energy Materials & Solar Cells》2011,95(2):791-796
Copper indium disulfide (CuInS2) thin films have been successfully prepared on Ni substrates using a novel one-step potentiostatic electrodeposition combined with a potassium hydrogen phthalate (C8H5KO4) complexing agent, accompanied by annealing at 350 °C. Electrodeposition in the solution of Cu and In salts and sodium thiosulfate (Na2S2O3) containing an adequate concentration of C8H5KO4 (e.g., [C8H5KO4]=23 mM) provides thin films comprised of a CuInS2 single phase as the bulk composition, without forming CuxS secondary phases. In addition to the effect on bulk-phase compositions, the adjustment of [C8H5KO4] causes variation in morphology and atomic composition of the film surface. The surface states of the films change from the Cu-rich rough surface at low [C8H5KO4] (15 mM) to the In-rich smooth surface at high [C8H5KO4] (23 mM). The higher [C8H5KO4] induces the grains constructing the film to interconnect and form a densely packed CuInS2 film without voids and pinholes. The single-phase and void-free CuInS2 film shows a band gap of 1.54 eV, satisfying the requirement of the absorber layers in solar cells. The electrical properties tests denote its n-type conductivity with a resistivity of 9.6×10−5 Ω cm, a carrier concentration of 2.9×1021 cm−3 and a carrier mobility of 22.2 cm2 V−1 s−1. 相似文献
8.
One-step electrodeposition using sodium thiosulfate (Na2S2O3) as a sulfur source has been studied for the preparation of Cu---In---S thin films. A deposited film is found to have a sufficiently high sulfur content compared with films deposited using thiourea as a sulfur source. The film deposited using Na2S2O3 is also found to have an excellent morphology compared with electrodeposited Cu---In precursors. Predominant factors to govern film composition, In/Cu and S/(Cu + In) ratios, are also investigated in this study. An HC1 content added in order to decompose S2O32− ions in the solution is found to be one of the important factors to control composition of deposited films. A sulfur cocentration in the solution influences not only S/(Cu + In) ratio but also In/Cu ratio in the film. Reproducibility of film composition is deteriorated as the solution temperature increases. 相似文献
9.
I. Luck J. Kneisel K. Siemer J. Bruns R. Scheer R. Klenk N. Janke D. Brunig 《Solar Energy Materials & Solar Cells》2001,67(1-4)
Using different glass substrate types the Na content in sequentially and Cu-rich prepared CuInS2 films and corresponding CuInS2/CdS/ZnO thin-film solar cells is varied. The purpose was to investigate the influence of different Na concentrations on absorbers and devices. While the morphology of the absorbers seems not to be affected by this variation, corresponding PL spectra differ significantly. The properties of the solar cells, however, show no dependence on the Na concentration. This implies that even though the defect chemistry of CuInS2, sequentially prepared under Cu excess, is changed by the presence of Na this influence has no impact on properties of corresponding solar cells. 相似文献
10.
J. SandinoE. Romero J.S. OyolaG. Gordillo H. Lichte 《Solar Energy Materials & Solar Cells》2011,95(8):2006-2009
This work presents results from a study carried out on the Mo/CuInS2/ZnS stacked layers, using high-resolution transmission electron microscopy (HRTEM). This system will be used later for the fabrication of solar cells with Mo/CuInS2/ZnS/TCO structure, where the layers conforming it will perform as an electrical contact, absorber layer and buffer layer, respectively. The layers of the Mo/CuInS2/ZnS system were deposited sequentially on soda lime glass substrates. The Mo film was deposited by DC magnetron sputtering, the CuInS2 (CIS) layer was grown by co-evaporation of precursors in a two-stage process and the ZnS was deposited by co-evaporation and by CBD (chemical bath deposition) using a solution containing zinc acetate, sodium citrate, ammonia and thiourea.The performed study provided significant information regarding crystalline structure, grain boundaries and defects visualization of each one of the layers as well as of the Mo/CuInS2 and CuInS2/ZnS interfaces. 相似文献
11.
Preparation and properties of CuInS2 thin film prepared from electroplated precursor 总被引:1,自引:1,他引:1
Yoshio Onuma Kenji Takeuchi Sumihiro Ichikawa Yasunari Suzuki Ryo Fukasawa Daisuke Matono Kenji Nakamura Masao Nakazawa Koji Takei 《Solar Energy》2006,80(1):132-138
Thin CuInS2 films were prepared by sulfurization of Cu/In bi-layers. First, the precursor layer was electroplated onto the treated surface of Mo-coated glass. Observation of the cross-section prepared by focused ion beam (FIB) etching revealed that the void-free film was initially formed on the top surface of the precursor layer and continued to grow until the advancing front of the film reached the Mo layer. The nucleation of voids near the bottom of the CuInS2 film followed. To determine whether the condition of the Cu/In alloy influences the CuInS2 quality we investigated the Cu/In alloy state using FIB. We found that the annealed precursor of low Cu/In ratio (1.2) has several voids in the mid position in the layer compared with Cu-rich precursor (1.6). The cross-sectional view of the Cu-rich absorber layer is uniform compared with the low copper absorber layer. Thin film solar cells were fabricated using the CuInS2 film (Cu/In ratio: 1.2) as an optical absorber layer. It was found that the optimization of a sulfurization period is important in order to improve the cell efficiency. We have not yet obtained good results with high Cu-rich absorber because of a blister problem. This blister was found before sulfurization. So, we are going to solve this blister problem before sulfurization. 相似文献
12.
Yoshio Onuma Kenji Takeuchi Sumihiro Ichikawa Mina Harada Hiroko Tanaka Ayumi Koizumi Yumi Miyajima 《Solar Energy Materials & Solar Cells》2001,69(3)
The CuInS2 films with a maximum thickness of about 9 μm and a maximum atomic Cu/In ratio (as-deposited precursor) of 3.0 were prepared, and, to prevent peeling from substrate, were heat treated during Cu/In evaporation and/or intercalated with very thin Pt or Pd (between Mo and CuInS2 layers). Thus, we could prepare the films with very large grain. It is also worth noting that the large grain films were easily optimized by chemical etching of the films using a thick film and Cu-rich composition. Therefore, the absorber for high-efficiency solar cells can be prepared by varying over a wide range of composition and thickness of precursor. The characterization of CuInS2 absorbers with various film thickness and compositions were investigated and related with the performance of the photovoltaic device. 相似文献
13.
Teny Theresa John Meril Mathew C. Sudha Kartha K.P. Vijayakumar T. Abe Y. Kashiwaba 《Solar Energy Materials & Solar Cells》2005,89(1):27-36
Copper indium sulfide (CuInS2)/In2S3 solar cells were fabricated using spray pyrolysis method and high short circuit current density and moderate open circuit voltage were obtained by adjusting the condition of deposition and thickness of both the layers. Consequently, a relatively high efficiency of 9.5% (active area) was obtained without any anti-reflection coating. The cell structure was ITO/CuInS2/In2S3/Ag. We avoided the usual cyanide etching and CdS buffer layer, both toxic, for the fabrication of the cell. 相似文献
14.
ZnO buffer layers were grown by a chemical-bath deposition (CBD) in order to improve the interface quality in p-CuInS2 based solar cells, to improve the light transmission in the blue wavelength region, but also as an alternative to eliminate the toxic cadmium. The process consists of immersion of different substrates (glass, CIS) in a dilute solution of tetraamminezinc II, [Zn(NH2)4]2+, complex at 60–95°C. During the growth process, a homogeneous growth mechanism which proceeds by the sedimentation of a mixture of ZnO and Zn(OH)2 clusters formed in solution, competes with the heterogeneous growth mechanism. The mechanism consists of specific adsorption of a complex Zn(II) followed by a chemical reaction. The last process of growth results in thin, hard, adherent and specularly reflecting films. The characterization of the deposited CBD-ZnO layers was performed by X-ray diffraction (XRD), optical transmittance, scanning electron microscopy, transmission electron microscopy (TEM) and X-ray photoelectron spectroscopy (XPS). The as-deposited films on glass show hexagonal zincite structure with two preferred orientations (1 0 0) and (1 0 1). High optical transmittance up to 80% in the near-infrared and part of the visible region was observed. The low growth rate of the films on CIS suggests an atomic layer-by-layer growth process.The device parameters and performance are compared to heterojunction with a standard CdS buffer layer. 相似文献
15.
P. Guha D. Das A. B. Maity D. Ganguli S. Chaudhuri 《Solar Energy Materials & Solar Cells》2003,80(1):115-130
CuInS2 powder was prepared by wet chemical route. The chalcopyrite structure of the powder was revealed by XRD studies. Raman measurements of the powder sample indicated four prominent peaks at 292, 305, 340 and 472 cm−1. The possible origin of the 305 cm−1 peak was investigated and was found to be some local vibration in the structure. The peaks at 292 and 340 cm−1 were ascribed to A1 and B2 modes, respectively. The peak at 472 cm−1 which was due to the formation of SO4−2 ion at lower pH value of the precursor solution could be eliminated by using pH>11.0. Photoluminescence (PL) studies of the CuInS2 powder indicated two distinct peaks at 1.49 and 1.42 eV. Post deposition annealing treatment in H2 atmosphere revealed the formation of excess sulphur vacancy leading to the peak at 1.42 eV in the PL spectra while O2 annealing of the powder created a deep defect level at 1.10 eV. Thick CuInS2 films were prepared by Doctor's blade technique. Optical transmittance studies of these films indicated direct allowed transition at 1.5 eV. 相似文献
16.
Takayuki Negami Yasuhiro Hashimoto Mikihiko Nishitani Takahiro Wada 《Solar Energy Materials & Solar Cells》1997,49(1-4)
CuInS2 thin-films were prepared by sulfurization of Cu---In---O precursors in H2S gas. X-ray diffraction patterns showed that In2O3 phases did not remain in the CuInS2 films sulfurized in a H2S and H2 atmosphere, whereas In2O3 phase remained in the films sulfurized in a H2S and Ar atmosphere. The performance of CuInS2 solar cells were studied as a function of the H2 gas pressure during sulfurization. The open-circuit voltage, short-circuit current and fill factor increased with increasing the H2 gas pressure. The conversion efficiency of the CuInS2 solar cells is strongly affected by the reduction of the Cu---In---O precursors. 相似文献
17.
M. D. Kannan R. Balasundaraprabhu S. Jayakumar P. Ramanathaswamy 《Solar Energy Materials & Solar Cells》2004,81(3):379
A simple close-spaced vapour transport (CSVT) system has been designed and fabricated. Copper indium diselenide (CuInSe2) thin films of wide range of thickness (4000–60000 Å) have been prepared using the fabricated CSVT system at source temperatures 713, 758 and 843 K. A detailed study on the deposition temperature has been made and the temperature profile along with the reaction kinetics is reported. The composition of the chemical constituents of the films has been determined by energy dispersive X-ray analysis. The structural characterization of the as-deposited CuInSe2 films of various thicknesses has been carried out by X-ray diffraction method. The diffractogram revealed that the CuInSe2 films are polycrystalline in nature with chalcopyrite structure. The structural parameters such as lattice constants, axial ratio, tetragonal distortion, crystallite size, dislocation density and strain have been evaluated and the results are discussed. The surface morphology of the as-deposited CuInSe2 thin films has been studied using scanning electron microscope. The transmittance characteristics of the CuInSe2 films have been studied using double beam spectrophotometer in the wavelength range 4000–15000 Å and the optical constants n and k are evaluated. The absorption coefficient has been found to be very high and is of the order of 105–106 m−1. CuInSe2 films are found to have a direct allowed transition and the optical band gap is found to be in the range 0.85–1.05 eV. 相似文献
18.
CuGaSe2 thin films with thicknesses of about 2 μm were prepared by flash and single source evaporation onto mica and (1 1 0)-oriented ZnSe substrates in the substrate temperature range 150–450°C. The obtained polycrystalline CuGaSe2 films had the chalcopyrite structure with the predominant growth direction 2 2 1. Hall effect, conductivity and luminescence measurements have been carried out on CuGaSe2 thin films and source materials: CuGaSe2 single crystals grown by Bridgman technique and by chemical vapour transport using I2 as transport agent. All films and crystals are p-type. Two acceptor levels with ionization energies EA150–56 meV and EA2130–150 meV have been identified as due to Ga vacancy and presence of Se atoms on interstitial sites respectively. 相似文献
19.
Optimization of substrate temperature of spray pyrolysed CuInS2 absorber is discussed along with its effect on the photoactivity of junction fabricated. For CuInS2 thin films, properties like crystallinity, thickness and composition showed progressive behavior with substrate temperature. X-ray photoelectron spectroscopic depth profile of all the samples showed that the concentration of copper on the surface of the films is significantly lesser than that in the bulk thus avoiding need for toxic cyanide etching. Interestingly, samples prepared at 623 K had higher conductivity compared to those prepared above and below this temperature. Also, the low energy transition, in addition to the direct band gap which was observed in other samples were absent in films prepared at 623 K. From thermally stimulated conductivity studies it was seen that shallow levels present in this sample contribute to its improved conductivity. Also, CuInS2/In2S3 bilayer prepared at this substrate temperature showed higher photoactivity than those prepared at other temperatures. 相似文献
20.
B. Asenjo A.M. Chaparro M.T. Gutierrez J. Herrero J. Klaer 《Solar Energy Materials & Solar Cells》2005,87(1-4):647
Solar cells of CuInS2/In2S3/ZnO type are studied as a function of the In2S3 buffer deposition conditions. In2S3 is deposited from an aqueous solution containing thioacetamide (TA), as sulfur precursor and In3+. In parallel, variable amounts of In2O3 are deposited that have an important influence on the buffer layer behavior. Starting from deposition conditions determined in a preliminary study, a set of parameters is chosen to be most determining for the buffer layer behavior, namely the solution temperature, the concentration of thioacetamide [TA], and the buffer thickness. The solar cell results are discussed in relation with these parameters. Higher efficiency is attained with buffer deposited at high temperature (70 °C) and [TA] (0.3 M). These conditions are characterized by short induction time, high deposition rate and low In2O3 content in the buffer. On the other hand, the film deposited at lower temperature has higher In2O3 content, and gives solar cell efficiency sharply decreasing with buffer thickness. This buffer type may attain higher conversion efficiencies if deposited on full covering very thin film. 相似文献