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Cadmium telluride, CdTe, is now firmly established as the basis for the market-leading thin-film solar-cell technology. With laboratory efficiencies approaching 20 per cent, the research and development targets for CdTe are to reduce the cost of power generation further to less than half a US dollar per watt (ref. 2) and to minimize the environmental impact. A central part of the manufacturing process involves doping the polycrystalline thin-film CdTe with CdCl2. This acts to form the photovoltaic junction at the CdTe/CdS interface and to passivate the grain boundaries, making it essential in achieving high device efficiencies. However, although such doping has been almost ubiquitous since the development of this processing route over 25 years ago, CdCl2 has two severe disadvantages; it is both expensive (about 30 cents per gram) and a water-soluble source of toxic cadmium ions, presenting a risk to both operators and the environment during manufacture. Here we demonstrate that solar cells prepared using MgCl2, which is non-toxic and costs less than a cent per gram, have efficiencies (around 13%) identical to those of a CdCl2-processed control group. They have similar hole densities in the active layer (9 × 1014 cm−3) and comparable impurity profiles for Cl and O, these elements being important p-type dopants for CdTe thin films. Contrary to expectation, CdCl2-processed and MgCl2-processed solar cells contain similar concentrations of Mg; this is because of Mg out-diffusion from the soda-lime glass substrates and is not disadvantageous to device performance. However, treatment with other low-cost chlorides such as NaCl, KCl and MnCl2 leads to the introduction of electrically active impurities that do compromise device performance. Our results demonstrate that CdCl2 may simply be replaced directly with MgCl2 in the existing fabrication process, thus both minimizing the environmental risk and reducing the cost of CdTe solar-cell production. [ABSTRACT FROM AUTHOR]

The processes of the noncatalytic synthesis of structures with CdTe nanowires by magnetron sputtering deposition are studied. It is shown that the deposition of magnetron sputtered CdTe onto substrates covered by a porous SiO layer can result in CdTe nanowires formation. The porosity of SiO layers with thicknesses from 2 to 15 nm fabricated by magnetron sputtering deposition is estimated. [ABSTRACT FROM AUTHOR]

We have investigated CdTe/CdS/In2O3:F/glass solar cell structures using quantitative SIMS for profiling the impurity distribution from the CdTe free surface through to the glass substrate. Ion implanted CdTe standards were used. The effect of the purity of the CdTe starting material was determined by studying two structures grown from 7N and 5N source materials. Particular emphasis was placed on the potentially electrically active impurities that may originate from the CdTe starting material, and are likely to affect the CdTe/CdS solar cell performance. It was shown that Cu, Zn, Sn, Sb and Pb profiles had the same level and shape in the CdTe layer regardless of the purity of the starting material used, and were therefore not originating from the starting material. Cl, O, Na and Si showed higher levels for structures grown using 5N purity CdTe compared to those from 7N, and may, at least in part, be due to the CdTe starting material used. It was also postulated that at least some impurities (in addition to Cl) may partially come from the CdCl2 treatment, and/or from the TCO (In) and glass (for Si and Na). Te and S interdiffusion at the CdTe/CdS interface was also shown to be enhanced when 5N CdTe source material is used as compared to 7N. [ABSTRACT FROM AUTHOR]

We have used low temperature photoluminescence (PL) to study thin film CdTe/CdS solar cell structures. The devices were produced by close space sublimation (CSS) and have undergone a post-growth treatment, a vital step in increasing device efficiency. The treatment consisted of evaporating a thin layer of CdCl2 onto the back CdTe surface and heat treating in air at 400 °C for between 10 and 120 min. This produced a range of device efficiencies from 2% to 9%. The efficiency improvements are the result of a complex interaction between the CdCl2, impurities and sulfur interdiffusion. The structures were prepared for PL by a chemical bevel etching technique which allows the luminescence emission to be studied as a function of depth throughout the sample. The main features in the PL spectra have been identified as being due to the Cl-A center and the Te-dislocation-related Y luminescence band. Using PL we have quantified the S diffusion into the CdTe which has a maximum of 20% at the interface in the most efficient samples. We have also obtained the profiles of recombination and non-radiative recombination centers in the device. We observe correlations between impurity centers and device efficiency which can help explain the effects of the CdCl2 treatment on the optoelectronic properties of the CdTe/CdS junction. [ABSTRACT FROM AUTHOR]

In this study, we have investigated the microstructural and optical properties of thin films of CuCl grown by vacuum evaporation on amorphous silica glass, polycrystalline indium tin oxide (ITO) and Silicon (100) substrates. Room temperature X-ray diffraction measurements reveal that CuCl grows preferentially with a (111) orientation irrespective of the substrate. Atomic force microscopy measurements showed similar surface topologies and roughness for CuCl/Si, CuCl/ITO and CuCl/Glass structures. Photoluminescence measurements at 20 K revealed the bound bi-exciton N1, impurity bound exciton I1 and the free exciton Z3 occurring at 3.152 ± 0.002 eV, 3.18 eV, and 3.204 eV, respectively, for all three structures. In addition to this, temperature dependent impedance measurements using irreversible electrodes (Au) showed that the deposited CuCl is a mixed ionic and electronic semiconductor with a predominantly extrinsic cationic conduction mechanism at temperatures above ∼280 K and with electronic conduction dominant at temperatures below ∼265 K. [ABSTRACT FROM AUTHOR]