Ion-beam synthesis of zinc-based nanoparticles in SiO2

In this paper production process of Zn nanocrystals in SiO2 by using an implantation of high dose zinc ions with energy of 130 keV and annealing process in 700°C were described. Using electron microscopy was established that annealing causes extension of admixtures distribution on depth and zinc nanoparticles size increasing from approx. 1 - 6 nm to 12 - 18 nm. For prepared material AC conductivity measurements were made in temperatures range from liquid nitride temperature (LNT) to 373 K and at frequencies range from 50 Hz to 5 MHz. Strong frequency dependence on conductivity proves that in this nanocomposite Zn-SiO2 conduction takes place by electron hopping exchange (tunneling) between metallic phase nanoparticles. It was established that three activation energies of conductivity occurs in temperatures range of LNT – 373 K – in low temperatures ΔE1≈0.001 eV, in medium temperatures ΔE2≈0.025 eV and in higher temperatures area ΔE3≈0.096 eV. This is due to the presence of at least two types of nanoparticles. First there are zinc nanoparticles with zinc oxide coating, second there are nanoparticles without the coating. The highest activation energy occurs during electrons tunneling between nanoparticles with zinc oxide coating. Intermediate activation energy corresponds to tunneling from nanoparticle with coating to nanoparticle without coating or conversely. The lowest activation energy corresponds to electrons hopping between nanoparticles without coatings.

[1]  Pascal Normand,et al.  Charge storage and interface states effects in Si-nanocrystal memory obtained using low-energy Si+ implantation and annealing , 2000 .

[2]  Marek Opielak,et al.  Formation process of spheroidal particles of gold and nanophases formation in AlN-TiB2-TiSi2 coatings after annealing with subsequent implantation , 2015 .

[3]  Uwe Rau,et al.  Microcrystalline silicon-oxygen alloys for application in silicon solar cells and modules , 2013 .

[4]  Vitalii Bondariev,et al.  The effect of annealing on induction like properties of (FeCoZr)x(CaF2)(100−x) nanocomposite films produced by ion-beam sputtering in the vacuum environment , 2015 .

[5]  M. Opielak,et al.  Structure and Properties of Multilayer Nanostructured Coatings TiN/MoN Depending on Deposition Conditions , 2014 .

[6]  Vitalii Bondariev,et al.  Annealing of (CoFeZr)x(CaF2)100-xNanocomposites Produced by the Ion-Beam Sputtering in the Ar and O2Ambient , 2013 .

[7]  A. K. Jonscher,et al.  Electronic processes in non-crystalline materials: By N. F. Mott and E. A. Davis, Clarendon Press: Oxford Univ. Press, Oxford, 1971; 437 pp. Price: £7.50 , 1972 .

[8]  A. K. Fedotov,et al.  Hopping of electron transport in granular Cux(SiO2)1–x nanocomposite films deposited by ion-beam sputtering , 2014 .

[9]  H. Hofmeister,et al.  Raman scattering and photoluminescence from Si nanoparticles in annealed SiOx thin films , 2002 .

[10]  C. Glover,et al.  Disorder in Au and Cu nanocrystals formed by ion implantation into thin SiO2 , 2005 .

[11]  T. Kołtunowicz,et al.  Voltage and Current Resonance in Nanocomposite (FeCoZr)_x(CaF₂)_{100-x} Produced by Ion-Beam Sputtering in Pure Argon Atmosphere , 2015 .

[12]  A. Fedotov,et al.  Carrier transport in porous-Si/Ni/c-Si nanostructures , 2016 .

[13]  Karazin Kharkiv,et al.  The Influence of the Ion Implantation of Au- to the Microstructure of the Amorphous-nanocrystaline AlN-TiB2-TiSi2 , 2015 .

[14]  Guo-Qiang Lo,et al.  Improved dye-sensitized solar cells with a ZnO-nanoflower photoanode , 2007 .

[15]  T. Kołtunowicz Test Station for Frequency-Domain Dielectric Spectroscopy of Nanocomposites and Semiconductors , 2015 .

[16]  Oleksandr Viacheslavovych Bondar,et al.  Structure and properties of arc evaporated nanoscale TiN/MoN multilayered systems , 2015 .

[17]  F. Komarov,et al.  Effects of surfactant and fabrication procedure on the electrical conductivity and electromagnetic shielding of single‐walled carbon nanotube films , 2015 .

[18]  Tomasz N. Koltunowicz,et al.  Inductive type properties of FeCoZr–CaF2 and FeCoZr–PZT nanocomposites , 2015, Journal of Materials Science: Materials in Electronics.

[19]  G. Lo,et al.  Enhanced field emission from injector-like ZnO nanostructures with minimized screening effect , 2007, Nanotechnology.

[20]  S. Güner,et al.  Optical properties of Ag nanoclusters formed by irradiation and annealing of SiO2/SiO2:Ag thin films , 2014 .

[21]  P. Zhukowski,et al.  Magnetic properties of nanocomposites (CoFeZr)x(Al2O3)1-x , 2010 .

[22]  A. Pogrebnjak,et al.  The structure and properties of high-entropy alloys and nitride coatings based on them , 2014 .

[23]  Vitalii Bondariev,et al.  Enhancement of negative capacitance effect in (CoFeZr)x(CaF2)(100−x) nanocomposite films deposited by ion beam sputtering in argon and oxygen atmosphere , 2014 .

[24]  O. Boiko,et al.  AC Hopping Conductance in Nanocomposite Films with Ferromagnetic Alloy Nanoparticles in a PbZrTiO3 Matrix , 2015, Journal of Electronic Materials.

[25]  H. Ahmed,et al.  Metal-based single electron transistors , 1997 .

[26]  A. K. Fedotov,et al.  Influence of sputtering atmosphere on hopping conductance in granular nanocomposite (FeCoZr)x(Al2O3)1−x films , 2014 .

[27]  O. Ivasishin,et al.  Irradiation resistance, microstructure and mechanical properties of nanostructured (TiZrHfVNbTa)N coatings , 2016 .

[28]  J. Misiewicz,et al.  Mechanism of enhanced photoluminescence of Tb ions in hydrogenated silicon-rich silicon oxide films , 2016 .

[29]  Tomasz N. Koltunowicz,et al.  Correlation between local Fe states and magnetoresistivity in granular films containing FeCoZr nanoparticles embedded into oxygen-free dielectric matrix , 2014 .

[30]  Sheng Chu,et al.  Electrically pumped ultraviolet ZnO diode lasers on Si , 2008 .

[31]  Marek Opielak,et al.  Mechanical Properties of Zn-Ni-SiO_2 Coating Deposited under X-ray Irradiation , 2014 .

[32]  T. Kołtunowicz,et al.  Dielectric Properties of (CoFeZr)_x(PZT)_{100-x} Nanocomposites Produced with a Beam of Argon and Oxygen Ions , 2014 .