Marko Yli-Koski
Aalto University
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Publication
Featured researches published by Marko Yli-Koski.
IEEE Journal of Photovoltaics | 2013
Päivikki Repo; Antti Haarahiltunen; Lauri Sainiemi; Marko Yli-Koski; Heli Talvitie; Martin C. Schubert; Hele Savin
The poor charge-carrier transport properties attributed to nanostructured surfaces have been so far more detrimental for final device operation than the gain obtained from the reduced reflectance. Here, we demonstrate results that simultaneously show a huge improvement in the light absorption and in the surface passivation by applying atomic layer coating on highly absorbing silicon nanostructures. The results advance the development of photovoltaic applications, including high-efficiency solar cells or any devices, that require high-sensitivity light response.
Journal of Applied Physics | 2007
Antti Haarahiltunen; Hele Väinölä; O. Anttila; Marko Yli-Koski; J. Sinkkonen
Heterogeneous iron precipitation in silicon was studied experimentally by measuring the gettering efficiency of oxide precipitate density of 1×1010cm−3. The wafers were contaminated with varying iron concentrations, and the gettering efficiency was studied using isothermal annealing in the temperature range from 300to780°C. It was found that iron precipitation obeys the so-called s-curve behavior: if iron precipitation occurs, nearly all iron is gettered. For example, after 30min annealing at 700°C, the highest initial iron concentration of 8×1013cm−3 drops to 3×1012cm−3, where as two lower initial iron concentrations of 5×1012 and 2×1013cm−3 remain nearly constant. This means that the level of supersaturation plays a significant role in the final gettering efficiency, and a rather high level of supersaturation is required before iron precipitation occurs at all. In addition, a model is presented for the growth and dissolution of iron precipitates at oxygen-related defects in silicon during thermal proces...
Journal of Applied Physics | 2009
Antti Haarahiltunen; Hele Savin; Marko Yli-Koski; Heli Talvitie; J. Sinkkonen
We propose a quantitative model for phosphorus diffusion gettering (PDG) of iron in silicon, which is based on a special fitting procedure to experimental data. We discuss the possibilities of the underlying physics of the segregation coefficient. Finally, we show that the proposed PDG model allows quantitative analysis of gettering efficiency of iron at various processing conditions.
Applied Physics Letters | 2009
Hele Savin; Marko Yli-Koski; Antti Haarahiltunen
We investigate the impact of copper on the light induced minority-carrier lifetime degradation in various crystalline silicon materials. We demonstrate here that the presence of neither boron nor oxygen is necessary for the degradation effect. In addition, our experiments reveal that copper contamination alone can cause the light induced minority-carrier lifetime degradation.
Journal of Applied Physics | 2011
Heli Talvitie; Ville Vähänissi; Antti Haarahiltunen; Marko Yli-Koski; Hele Savin
We have studied experimentally the phosphorus diffusion gettering (PDG) of iron in monocrystalline silicon at the temperature range of 650–800 °C. Our results fill the lack of data at low temperatures so that we can obtain a reliable segregation coefficient for iron between a phosphorus diffused layer and bulk silicon. The improved segregation coefficient is verified by time dependent PDG simulations. Comparison of the PDG to boron diffusion gettering (BDG) in the same temperature range shows PDG to be only slightly more effective than BDG. In general, we found that BDG requires more carefully designed processing conditions than PDG to reach a high gettering efficiency.
Journal of The Electrochemical Society | 2003
Hele Väinölä; Marko Yli-Koski; Antti Haarahiltunen; J. Sinkkonen
12 cm 23 can be detected by this method. It is demonstrated that positive corona charge can be used to prevent out-diffusion of interstitial copper, while negative charge enables copper to freely diffuse to the wafer surfaces. It was observed that the precipitation rate of copper increased significantly when the bias-light intensity is raised above a certain critical level. In addition, the copper precipitation rate was discovered to be much higher in samples which have internal gettering sites. These findings suggest that (i) high intensity light reduces the electrostatic repulsion between positively charged interstitial copper ions and copper precipitates enabling copper to precipitate in the wafer bulk even at a low concentration level, and ( ii) during high intensity illumination, oxygen precipitates provide effective heterogeneous nucleation sites for copper.
Applied Physics Letters | 2008
Antti Haarahiltunen; Heli Talvitie; Hele Savin; Marko Yli-Koski; Muhammad Imran Asghar; J. Sinkkonen
In this paper, a model is presented for boron diffusion gettering of iron in silicon during thermal processing. In the model, both the segregation of iron due to high boron doping concentration and heterogeneous precipitation of iron to the surface of the wafer are taken into account. It is shown, by comparing simulated results with experimental ones, that this model can be used to estimate boron diffusion gettering efficiency of iron under a variety of processing conditions. Finally, the application of the model to phosphorus diffusion gettering is discussed.
Applied Physics Letters | 2005
Hele Väinölä; Eero Saarnilehto; Marko Yli-Koski; Antti Haarahiltunen; J. Sinkkonen; G. Berenyi; T. Pavelka
We propose a method to measure trace copper contamination in p-type silicon using the microwave photoconductivity decay (μ-PCD) technique. The method is based on the precipitation of interstitial copper, activated by high-intensity light, which results in enhanced minority carrier recombination activity. We show that there is a quantitative correlation between the enhanced recombination rate and the Cu concentration by comparing μ-PCD measurements with transient ion drift and total reflection x-ray fluorescence measurements. The results indicate that the method is capable of measuring Cu concentrations down to 1010cm−3. There are no limitations to wafer storage time if corona charge is used on the oxidized wafer surfaces as the charge prevents copper outdiffusion. We briefly discuss the role of oxide precipitates both in the copper precipitation and in the charge carrier recombination processes.
Journal of Applied Physics | 2014
Jeanette Lindroos; Yacine Boulfrad; Marko Yli-Koski; Hele Savin
Multicrystalline silicon (mc-Si) is currently dominating the silicon solar cell market due to low ingot costs, but its efficiency is limited by transition metals, extended defects, and light-induced degradation (LID). LID is traditionally associated with a boron-oxygen complex, but the origin of the degradation in the top of the commercial mc-Si brick is revealed to be interstitial copper. We demonstrate that both a large negative corona charge and an aluminum oxide thin film with a built-in negative charge decrease the interstitial copper concentration in the bulk, preventing LID in mc-Si.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2002
J. Härkönen; E. Tuominen; K. Lassila-Perini; M. Palokangas; Marko Yli-Koski; Victor Ovchinnikov; Paula Heikkilä; L. Palmu; S. Kallijärvi
Abstract Three sets of silicon microstrip detectors have been processed and characterized. Recombination lifetimes of each set have been measured by Microwave Photoconductivity Decay ( μ PCD) method. In the this method, the silicon is illuminated by a laser pulse that generates electron hole pairs. The transient of the decaying carrier concentration is monitored by using a microwave signal. The recombination lifetime is a measure of the material quality i.e., defect/impurity concentration which affects the detectors’ electrical properties. A correlation between the recombination lifetime and the leakage current has been observed and discussed. The leakage current density in the best devices was about 6 nA cm −2 at 40 V . The average lifetime in the monitor wafer of this set was about 6500 μs . In comparison, average lifetime less than 1000 μs resulted in leakage currents of more than 100 nA cm −2 .