Publications

The contamination from the air (the identification of the impurity phases and their thermal evolution) of Fe-14Cr-3W-0.4Ti-0.25Y(2)O(3) oxide dispersion-strengthened ferritic steel powders ball-milled for different times was evidenced by thermal analysis in correlation with X-ray diffraction and scanning electron microscopy. The powders loaded under an argon atmosphere and milled up to 170 h with and without interruption of the milling process were compared. A steady state of Fe-Cr alloying was reached within the first 12 h. The reflections corresponding to a new phase with an fcc-CrN structure were found in XRD patterns of powders milled for a long time with interruption. The differential thermal analysis of powders milled over 12 h with interruption shows an exothermic peak at 625.5-653 degrees C, ascribed to the coarsening of the fcc-CrN, and an endothermic reaction above 1000 degrees C accompanied by a mass loss in thermogravimetric analysis. (Cr,Fe)(2)O-3 and retained austenite were also found upon the heating of as-milled (with interruption) powders to different temperatures. The endothermic feature was associated with the decomposition of CrN accompanied by the degassing of N-2. The observed phenomenon was explained to be the manifestation of contamination with nitrogen and oxygen from the air during the milling; the rate of contamination with nitrogen was estimated to be 0.011 mass% h(-1). The contamination level depends on the degree of alloying at the moment of the interruption of milling process. The contamination of the powders milled without interruption of milling process was insignificant. The experimental conditions described in this work can be further developed for the removal of impurities (e.g. nitrogen, nitrides, oxides) from alloyed ferritic steel powders.

An experimental study on the radial spreading of the liquid from a virtually infinite reservoir onto a horizontal fabric sample was performed using a simple setup which is presented in two variants: One variant (the simplest) collects the images of the wet spot during the radial outward wicking and the other variant collects the images simultaneously with the monitoring of the weight decrease of the liquid reservoir. We notice that recording with a webcam gives advantages in the subsequent data processing. Afterward, the resulting image series were processed with routines developed in LabVIEW to determine the area of the wet spot. The programs are better adapted to the inhomogeneous and anisotropic structure specific to textiles than the existent edge-finding algorithms. The time dependence of the wet area provides information about the wicking kinetics and further, by modeling the data, to the possible mechanism. The experiments were performed using solutions of red (rhodamin 6B) or blue (brilliant blue E133) dyes in linen and polyester samples differing besides the chemical structure in the roughness of their surfaces as well. The data allow an easy comparison between the textile behavior. Determination of the mass loss of the test liquid might be useful especially for the colored fabrics. The infinite reservoir case is compared with that of the finite reservoir. (C) 2016 Elsevier B.V. All rights reserved.

The crystal structure, electronic and magnetic properties of predicted new full-Heusler compounds Zr(2)MnZ (Z=Al, Ga, In) were studied within the density functional theory (DFT) framework. These materials exhibit unique properties that connect the spin gapless semiconducting character with the completely compensated ferrimagnetism. Magnetically ordered Zr(2)MnZ (Z=Al, Ga, In) compounds crystallize in inverse Heusler structure are stable against decomposition and have zero magnetic moment per formula unit, in agreement with Slater-Pauling rule. The Zr2MnAl compound presents semiconducting properties with an energy band gap of 0.41 eV in the majority spin channel and a zero band gap in the minority spin channel. By substituting completely the Al in Zr2MnAl via Ga and In elements, semiconducting pseudo band gaps are formed in the majority spin channels due to different neighborhoods around the manganese atoms, which decreases the energy of Mn triple degenerated anti-bonding states. (C) 2016 Elsevier B.V. All rights reserved.

Within this study a matrix assisted pulsed laser evaporation technique was employed for deposition of CdS quantum dots onto TiO2 nanotubes. The number of laser pulses and laser fluence were varied to control the amount of CdS deposit. TiO2 nanotubes were obtained via anodization technique of sputtered Ti film on FTO glass. For CdS synthesis, dimethyl sulfoxide (DMSO) was used as a matrix of the target which absorbs radiation of KrF* laser (lambda=248 nm), then evaporates enabling the deposition of CdS quantum dots dispersed into DMSO. This study showed that the size of the CdS nanoparticles synthetized in DMSO can be controlled with microwave treatment that causes the release of S2- ions from DMSO for creation of CdS nuclei and/or their further growth. The optimization of CdS synthesis is achieved by varying the duration of the microwave treatment and the microwave power. The obtained TiO2 photo anodes with different amounts of CdS were assembled with PbS cathodes and the polysulfide electrolyte was injected between. The influence of amount of CdS deposit and the microwave treatment of CdS on photovoltaic performance of the fabricated solar cells were analyzed under AM1.5. The results showed that microwave treatment produced a Cd(S)-DMSO complex onto CdS nanoparticles which led to a higher current density of the solar cells obtained using microwave treated CdS target. Also, the increase of CdS content by increasing the number of laser pulses provided the enhance of I-V characteristics of the solar cells. (C) 2016 Elsevier Ltd and Techna Group S.r.l. All rights reserved.

BiFeO3 is one of the most promising multiferroic materials but undergoes two major drawbacks: low dielectric susceptibility and high dielectric loss. Here we report high in-plane dielectric permittivity (epsilon' similar to 2500) and low dielectric loss (tan delta < 0.01) obtained on Bi0.95Y0.05FeO3 films epitaxially grown on SrTiO3 (001) by pulsed laser deposition. High resolution transmission electron microscopy and geometric phase analysis evidenced nanostripe domains with alternating compressive/tensile strain and slight lattice rotations. Nanoscale mixed phase/domain ensembles are commonly found in different complex materials with giant dielectric/electromechanical (ferroelectric/relaxors) or magnetoresistance (manganites) response. Our work brings insight into the joined role of chemical pressure and epitaxial strain on the appearance of nanoscale stripe structure which creates conditions for easy reorientation and high dielectric response, and could be of more general relevance for the field of materials science where engineered materials with huge response to external stimuli are a highly priced target.

Large scale ZnO nanowire arrays were grown directly on zinc foils using the thermal oxidation in air method. The X-ray diffraction and reflectance investigations confirm that the as-grown nanowires properties are typical for ZnO having a hexagonal wurtzite crystalline structure and band-gap values between 3.2 and 3.3 eV. The scanning electron microscopy images prove that the density and the dimensions (diameter and length) of the ZnO nanowires can be tuned by controlling the oxidation temperature. Wettability studies reveal in the case of Zn foils a hydrophilic behavior with high water droplet adhesion which is transformed into a superhydrophobic one with low water droplet adhesion after the foils' surfaces are covered with ZnO nanowires. Obtaining functional surfaces with such interesting wetting properties using a simple, inexpensive and highly reproducible thermal oxidation in air technique is very attractive for anticorrosion coatings and self-cleaning applications. (C) 2016 Elsevier B.V. All rights reserved.

Dense (95-98.6%) bulk boron carbide prepared by Spark Plasma Sintering (SPS) in Ar or N-2 atmospheres were subject to three-point flexural tests at room and at 1600 degrees C. Eight different consolidation conditions were used via SPS of commercially available B4C powder. Resulting specimens had similar grain size not exceeding 4 mu m and room-temperature bending strength (sigma(25) (degrees C)) of 300-600 MPa, suggesting that difference in sigma(25) (degrees C) m is due to development of secondary phases in monolithic boron carbide ceramics during SPS processing. To explain such difference the composition of boron carbide and secondary phases observed by XRD and Raman spectroscopy. The variation in intensity of the Raman peak at 490 cm(-1) of boron carbide suggests modification of the boron carbide composition and a higher intensity correlates with a higher room temperature bending strength (sigma(25) (degrees C)) and Vickers hardness (HV). Secondary phases can modify the level of mechanical characteristics within some general trends that are not dependent on additives (with some exceptions) or technologies. Namely, HV increases, sigma(25) (degrees C) decreases, and the ratio sigma(1600 degrees C)/sigma(25 degrees C) (sigma(1600 degrees C) - bending strength at 1600 degrees C) is lower when fracture toughness (K-IC) is higher. The ratio sigma(1600 degrees C)/sigma(25 degrees C) shows two regions of low and high K-IC delimited by K-IC=4.1 MPa m(0.5): in the low K-IC region, boron carbide specimens are produced in nitrogen. (c) 2016 Elsevier Ltd and Techna Group S.r.l. All rights reserved.

High density monolithic boron carbide specimens with grain size of 3-5 mu m were consolidated by spark plasma sintering using identical heating conditions and Ar or N-2 atmospheres. The effect of impurities from two different raw powders on the flexural strength was revealed. The increase in flexural strength was observed up to 1600 degrees C. Specimens consolidated in nitrogen had a higher strength than that consolidated in argon. Samples had the room temperature strength ranging from 350 to 550 MPa. The high temperature strength of our samples exceeding 400 MPa is higher than that previously reported for polycrystalline monolithic B4C. The supporting cracking/strengthening mechanism was discussed and proposed. (C) 2016 The Ceramic Society of Japan. All rights reserved.

Graphene nanopowder (G) with average thickness particle size of about 6-8 nm was added to MgB2 commercial powder. Starting composition was (MgB2)((1-x))(G)(x),x = 0.0125, 0.025, 0.05. Processing was performed by Spark Plasma Sintering (SPS) technique. All added samples have high density (above 95%). The critical temperature (T-c) and the lattice parameter a (c-axis lattice parameter is constant) show a small variation suggesting that carbon substitution for boron is low. TEM observations show the presence of un-reacted graphene plates supporting the T-c and structural results. It also indicates that G-addition does not modify the MgB2 microstructure. Despite this, there is an optimum doped sample (MgB2)(0.9875)(G)(0.0125) for which the critical current density at temperatures below 25 K is slightly higher at high magnetic fields than for the pristine sample. The addition of G is found as one of the least effective C-source additions enhancing J(c). We discuss results as being strongly related to variation of the residual stress. (C) 2016 Elsevier Ltd. All rights reserved.