Materials Map

Discover the materials research landscape. Find experts, partners, networks.

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The Materials Map is an open tool for improving networking and interdisciplinary exchange within materials research. It enables cross-database search for cooperation and network partners and discovering of the research landscape.

The dashboard provides detailed information about the selected scientist, e.g. publications. The dashboard can be filtered and shows the relationship to co-authors in different diagrams. In addition, a link is provided to find contact information.

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Materials Map under construction

The Materials Map is still under development. In its current state, it is only based on one single data source and, thus, incomplete and contains duplicates. We are working on incorporating new open data sources like ORCID to improve the quality and the timeliness of our data. We will update Materials Map as soon as possible and kindly ask for your patience.

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Helsinki Institute of Physics

in Cooperation with on an Cooperation-Score of 37%

Topics

Publications (75/75 displayed)

  • 2024Wetting Properties of Black Silicon Layers Fabricated by Different Techniques3citations
  • 2024(invited talk) Sulfur-hyperdoped silicon by ultrashort laser processingcitations
  • 2024Contactless analysis of surface passivation and charge transfer at the TiO 2-Si interface2citations
  • 2024Detection of Microcracks in Cz-Si Wafer Manufacturing by Photoluminescence Imagingcitations
  • 2024Contactless analysis of surface passivation and charge transfer at the TiO 2-Si interface2citations
  • 2024Impact of post-ion implantation annealing on Se-hyperdoped Ge1citations
  • 2024Impact of post-ion implantation annealing on Se-hyperdoped Ge1citations
  • 2024Bridging the gap between surface physics and photonics2citations
  • 2024Contactless analysis of surface passivation and charge transfer at the TiO2-Si interface2citations
  • 2024(poster) ALD SiO2 provides efficient Ge surface passivation with a tailorable charge polaritycitations
  • 2024(poster) ALD SiO2 provides efficient Ge surface passivation with a tailorable charge polaritycitations
  • 2023Surface passivation of Germanium with ALD Al2O3: Impact of Composition and Crystallinity of GeOx Interlayer6citations
  • 2023(oral talk) Effective carrier lifetime in ultrashort pulse laser hyperdoped silicon: dopant concentration dependence and practical upper limitscitations
  • 2023Atomic Layer Deposition of Titanium Oxide-Based Films for Semiconductor Applications—Effects of Precursor and Operating Conditions4citations
  • 2023Understanding the multilevel phenomena that enables inorganic atomic layer deposition to provide barrier coatings for highly-porous 3-D printed plastic in vacuumscitations
  • 2023Understanding the multilevel phenomena that enables inorganic atomic layer deposition to provide barrier coatings for highly-porous 3-D printed plastic in vacuumscitations
  • 2023Excellent Responsivity and Low Dark Current Obtained with Metal-Assisted Chemical Etched Si Photodiode4citations
  • 2023Comparison of SiNx-based Surface Passivation Between Germanium and Silicon9citations
  • 2023Plasma-enhanced atomic layer deposited SiO2 enables positive thin film charge and surface recombination velocity of 1.3 cm/s on germanium5citations
  • 2023Chemical Excitation of Silicon Photoconductors by Metal-Assisted Chemical Etching8citations
  • 2023Chemical Excitation of Silicon Photoconductors by Metal-Assisted Chemical Etching8citations
  • 2023Status report on emerging photovoltaics14citations
  • 2023Status report on emerging photovoltaics14citations
  • 2023Atomic Layer Deposition of Titanium Oxide-Based Films for Semiconductor Applications–Effects of Precursor and Operating Conditions4citations
  • 2023Atomic Layer Deposition of Titanium Oxide-Based Films for Semiconductor Applications–Effects of Precursor and Operating Conditions4citations
  • 2023Quantifying the Impact of Al Deposition Method on Underlying Al2O3/Si Interface Quality2citations
  • 2023Is Carrier Mobility a Limiting Factor for Charge Transfer in Tio2/Si Devices? A Study by Transient Reflectance Spectroscopy6citations
  • 2022Electron Injection in Metal Assisted Chemical Etching as a Fundamental Mechanism for Electroless Electricity Generation22citations
  • 2022Electron Injection in Metal Assisted Chemical Etching as a Fundamental Mechanism for Electroless Electricity Generation22citations
  • 2022Perspectives on Black Silicon in Semiconductor Manufacturing: Experimental Comparison of Plasma Etching, MACE and Fs-Laser Etching32citations
  • 2022Millisecond-Level Minority Carrier Lifetime in Femtosecond Laser-Textured Black Silicon11citations
  • 2022Luminescent (Er,Ho)2O3 thin films by ALD to enhance the performance of silicon solar cells12citations
  • 2022(oral talk) Compatibility of Al-neal in processing of Si devices with Al2O3 layercitations
  • 2022Impact of doping and silicon substrate resistivity on the blistering of atomic-layer-deposited aluminium oxide9citations
  • 2021Luminescent (Er,Ho)2O3 thin films by ALD to enhance the performance of silicon solar cells12citations
  • 2021Efficient photon capture on germanium surfaces using industrially feasible nanostructure formation13citations
  • 2021Al-neal Degrades Al2O3 Passivation of Silicon Surface3citations
  • 2020Al2O3 Thin Films Prepared by a Combined Thermal-Plasma Atomic Layer Deposition Process at Low Temperature for Encapsulation Applications6citations
  • 2020Al 2 O 3 Thin Films Prepared by a Combined Thermal-Plasma Atomic Layer Deposition Process at Low Temperature for Encapsulation Applications6citations
  • 2020Modeling Field-effect in Black Silicon and its Impact on Device Performance10citations
  • 2020Passivation of Detector-Grade Float Zone Silicon with Atomic Layer Deposited Aluminum Oxide12citations
  • 2020Impact of doping and silicon substrate resistivity on the blistering of atomic-layer-deposited aluminium oxide9citations
  • 2020Vacuum Outgassing Characteristics of Unpigmented 3-D Printed Polymers Coated with ALD Alumina8citations
  • 2020Vacuum Outgassing Characteristics of Unpigmented 3-D Printed Polymers Coated with ALD Alumina8citations
  • 2019Effect of MACE Parameters on Electrical and Optical Properties of ALD Passivated Black Silicon28citations
  • 2019Compatibility of 3-D Printed Devices in Cleanroom Environments for Semiconductor Processing16citations
  • 2019Compatibility of 3-D Printed Devices in Cleanroom Environments for Semiconductor Processing16citations
  • 2019Passivation of Detector‐Grade FZ‐Si with ALD‐Grown Aluminium Oxide12citations
  • 2018Economic Advantages of Dry-Etched Black Silicon in Passivated Emitter Rear Cell (PERC) Photovoltaic Manufacturing29citations
  • 2018Economic Advantages of Dry-Etched Black Silicon in Passivated Emitter Rear Cell (PERC) Photovoltaic Manufacturing29citations
  • 2018Elucidation of Iron Gettering Mechanisms in Boron-Implanted Silicon Solar Cells1citations
  • 2018Moving Beyond p-Type mc-Si2citations
  • 2018Solubility and Diffusivity27citations
  • 2018Moving Beyond p-Type mc-Si: Quantified Measurements of Iron Content and Lifetime of Iron-Rich Precipitates in n-Type Silicon2citations
  • 2018Nanometer-scale depth-resolved atomic layer deposited SiO2 thin films analysed by glow discharge optical emission spectroscopy6citations
  • 2018Nanometer-scale depth-resolved atomic layer deposited SiO2 thin films analysed by glow discharge optical emission spectroscopy6citations
  • 2018Rapid thermal anneal activates light induced degradation due to copper redistribution7citations
  • 2018Metallized Boron-Doped Black Silicon Emitters For Front Contact Solar Cells1citations
  • 2018Metallized Boron-Doped Black Silicon Emitters For Front Contact Solar Cells1citations
  • 2017Predictable quantum efficient detector based on n-type silicon photodiodes19citations
  • 2017Electronic Quality Improvement of Highly Defective Quasi-Mono Silicon Material by Phosphorus Diffusion Gettering10citations
  • 2017Surface Passivation Properties of HfO2 Thin Film on n-Type Crystalline Si48citations
  • 2017Toward Effective Gettering in Boron-Implanted Silicon Solar Cells2citations
  • 2017Modeling of light-induced degradation due to Cu precipitation in p-type silicon. II. Comparison of simulations and experiments19citations
  • 2017Ozone-Based Atomic Layer Deposition of Al2O3 from Dimethylaluminum Chloride and Its Impact on Silicon Surface Passivation17citations
  • 2017Full recovery of red zone in p-type high-performance multicrystalline silicon6citations
  • 2017Surface passivation of black silicon phosphorus emitters with atomic layer deposited SiO2/Al2O3 stacks34citations
  • 2017Modeling of light-induced degradation due to Cu precipitation in p-type silicon. Pt.II: Comparison of simulations and experiments19citations
  • 2016Finite- vs. infinite-source emitters in silicon photovoltaics1citations
  • 2016Investigation of Al2O3 Passivation Layers by Photoluminescence Imaging under Applied Voltagecitations
  • 2014Iron Precipitation upon Gettering in Phosphorus-Implanted Czochralski Silicon and its Impact on Solar Cell Performance1citations
  • 2013Analyses of the evolution of iron-silicide precipitates in multicrystalline silicon during solar cell processing32citations
  • 2013Passivation of black silicon boron emitters with atomic layer deposited aluminum oxide23citations
  • 2012Modeling the size distribution of iron silicide precipitates in multicrystalline silicon1citations
  • 2004Simulations of Iron Re-Dissolution from Oxygen Precipitates in Cz-Silicon and its Impact on Gettering Efficiencycitations

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Chart of shared publication
Ayvazyan, Gagik
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  • Ayvazyan, Gagik
  • Liu, Xiaolong
  • Vardanyan, Arman
  • Hakhoyan, Levon
  • Seibt, Michael
  • Radfar, Behrad
  • Paulus, Simon
  • Niemeyer, Tobias
  • Schäfer, Sören
  • Koskinen, Vesa
  • Vähänissi, Ville
  • Kontermann, Stefan
  • Kearney, Patrick Mc
  • Mutschall, Doris
  • Serue, Michael
  • Pasanen, Hannu P.
  • Ali-Löytty, Harri
  • Khan, Ramsha
  • Tkachenko, Nikolai V.
  • Lähteenmäki, Jukka-Pekka
  • Mustonen, Katja
  • Berencen, Yonder
  • Kentsch, Ulrich
  • Zhou, Shengqiang
  • Mc Kearney, Patrick
  • Punkkinen, Marko
  • Kuzmin, Mikhail
  • Kokko, Kalevi
  • Hakkarainen, Teemu
  • Viheriälä, Jukka
  • Guina, Mircea
  • Tukiainen, Antti
  • Laukkanen, Pekka
  • Isometsä, Joonas
  • Liu, Hanchen
  • Leiviskä, Oskari
  • Fung, John
  • Fung, Tsun Hang
  • Lehtiö, Juha Pekka
  • Kokko, K.
  • Laukkanen, P.
  • Pasanen, Toni P.
  • Miettinen, Mikko
  • Rad, Zahra Jahanshah
  • Leiviska, Oskari
  • Vahanissi, Ville
  • Matkivskyi, Vladyslav
  • Tranell, Maria Gabriella
  • Wenner, Sigurd
  • Sabatino, Marisa Di
  • De Alwis, Chathura
  • Ekstrum, Craig
  • Marin, Giovanni
  • Mayville, Pierce J.
  • Rauha, Ismo T. S.
  • Pearce, Joshua M.
  • Karppinen, Maarit
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  • Chen, Kexun
  • Yli-Koski, Marko
  • Ayedh, Hussein M.
  • Oksanen, Jani
  • Li, Shengyang
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  • Di Sabatino, Marisa
  • Hanchen, Liu
  • Ott, Jennifer
  • Rosta, Kawa
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  • Mack, Iris
  • Soldano, Caterina
  • Pasanen, Hannu
  • Ayedh, Hussein
  • Valden, Mika
  • Saari, Jesse
  • Radevici, Ivan
  • Pälikkö, Elmeri
  • Lastusaari, Mika
  • Safdar, Muhammad
  • Aho, Arto
  • Ghazy, Amr
  • Garin, Moises
  • Gadda, Akiko
  • Ylivaara, Oili M. E.
  • Mizohata, Kenichiro
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  • Zhu, Zhen
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  • Istratov, A. A.
  • Zhang, P.
  • Weber, E. R.
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document

(oral talk) Compatibility of Al-neal in processing of Si devices with Al2O3 layer

  • Ott, Jennifer
  • Vähänissi, Ville
  • Savin, Hele
  • Setälä, Olli E.
  • Pasanen, Toni P.
Abstract

Surface and bulk defects are a well-known reason for limited operation of silicon devices. These defects cause increased recombination and leakage current, and hence, their avoidance is an important factor in device processing. The traditional choice for surface passivation of silicon devices has been thermally grown silicon dioxide (SiO2). The development of device designs has led to increasing utilization of other thin films as well, including aluminum oxide (Al2O3). However, SiO2 is still often needed alongside Al2O3 in devices, such as induced junction detectors [1]. For effective elimination of defects, SiO2 typically needs to be annealed with a thin Al layer deposited on top of the thin film (so-called Al-neal process) [2]. If both SiO2 and Al2O3 are simultaneously present on the wafer, also the Al2O3 film will experience the Al-neal, which is usually performed as the last processing step in device fabrication. However, it has so far remained unresolved whether Al-nealing would have impact on the passivation performance of Al2O3, and hence, this needs to be studied.<br/><br/>Table 1 demonstrates the well-known result that Al-neal is highly beneficial in the case of SiO2 to reduce the interface defect density. Although Al-neal improves the carrier lifetime in SiO2-passivated Si by a factor of &gt;20, Al2O3 does not need Al-film for superior passivation, as it is provided by regular annealing already. This is mainly due to efficient field-effect passivation induced by the high density of negative fixed charges (see Table 1). However, Figure 1 reveals that the Al-neal process required for SiO2-passivated regions is detrimental for the passivation performance of Al2O3. Especially, if the Al2O3 film has already been annealed once before Al-neal, the lifetime in the Al2O3-passivated regions is reduced by an order of magnitude. Al-nealing Al2O3 directly after its deposition without a separate post-deposition anneal provides good surface passivation but cannot reach the lifetimes achieved without Al-nealing. <br/><br/>The root causes for such behavior are further investigated by separately examining the substeps of Al-nealing and their impact on the passivation performance of Al2O3 film. The two details that set the Al-neal apart from a regular annealing treatment are sputtering of Al on top of Al2O3 and the presence of this Al during annealing. To study the impact of these steps individually, the above experiment is repeated following the same process with the exception that Al is etched from top of Al2O3 before the final annealing. The obtained lifetimes are slightly higher than after Al-nealing but still far from the case without any sputtering (see Table 2), which proves that sputtering damage does indeed have an impact on passivation. Furthermore, the discrepancy still exists between cases with and without separate post-deposition annealing performed prior Al-nealing. This result indicates that sputtering damage can only partly explain the degraded passivation performance during the Al-neal of Al2O3. Another affecting factor could be depletion of hydrogen from the Al2O3 film during multiple annealings. This could result in annealed film not having enough hydrogen left to re-passivate the Si/Al2O3 interface after being damaged by sputtering. The presented findings can be considered in process design to achieve higher performance in silicon devices involving both Al2O3 and SiO2. Subsequently, we have already utilized the optimized Al-neal parameters in fabrication of Si detectors resulting in lower leakage current in the devices.<br/>References:<br/>[1] M. A. Juntunen, J. Heinonen, V. Vähänissi, P. Repo, D. Valluru, H. Savin, Nat. Photonics 10(12), 777-781 (2016).  <br/>[2] P. L. Castro, B. E. Deal, J. Electrochem. Soc. 118(2), 280 (1971).<br/>

Topics
  • Deposition
  • density
  • impedance spectroscopy
  • surface
  • experiment
  • thin film
  • aluminum oxide
  • aluminium
  • Hydrogen
  • Silicon
  • defect
  • annealing