National Institute Of Materials Physics - Romania

The source of collective magnetism in II-VI semiconductor quantum dots (QDs) doped with Mn2+ ions at high nominal impurity levels is still under debate. In the particular case of mesoporous, self-assembled cubic ZnS:Mn QDs, quantitative electron paramagnetic resonance (EPR) studies have shown that the Mn2+ ions incorporated in the core and on the surface of the QDs cannot be responsible for the observed collective magnetism because they remain in a diluted paramagnetic state up to the 50 000 ppm nominal concentration. Here we investigate the composition, localization, structure, and magnetic properties of the aggregates of Mn2+ ions incorporated in the mesoporous cZnS:Mn as a possible source of the observed collective magnetism. Samples of mesoporous cubic ZnS:Mn prepared by coprecipitation at several nominal impurity levels from 200 to 50 000 ppm are investigated by EPR, magnetometry, and analytical high resolution (scanning) transmission electron microscopy. The low temperature magnetic properties of the Mn2+ aggregates change from paramagnetic-like, for samples with nominal impurity levels up to 2000 ppm, to ones specific to larger clusters with distributed antiferromagnetic coupling at higher concentrations, behaving superparamagnetically above a certain temperature. There is also strong evidence that the Mn2+ aggregates responsible for the observed low temperature collective magnetism are incorporated as an amorphous phase of mainly Mn-Zn-O composition, localized in the interstices and pores of the mesoporous structure of the cubic ZnS:Mn QDs.

Vortex activation energy U-AC in the critical-state related AC magnetic response of superconductors (appearing in the vicinity of the DC irreversibility line) takes large values, as often reported, which is not yet understood. This behavior is essentially different from that of the vortex-creep activation energy at long relaxation time scales, and may become important for AC applications of superconductors. To elucidate this aspect, we investigated the AC signal of almost decoupled [YBa2Cu3O7](n)/[PrBa2Cu3O7](4) superlattices (with n = 11 or 4 units cells) in perpendicular DC and AC magnetic fields. In these model samples, the length of the hopping vortex segment is fixed by the thickness of superconducting layers and vortices are disentangled, at least at low DC fields. It is shown that the high U-AC values result from the large contribution of the pinning enhanced viscous drag in the conditions of thermally activated, non-diffusive vortex motion at short time scales, where the influence of thermally induced vortex fluctuations on pinning is weak. (C) 2016 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/).

Ex-situ spark plasma sintering (SPS) was used to obtain dense MgB2-based tapes in a Fe sheath with the starting composition (MgB2)(0.975) + (SiC)(0.025) + Te-0.01. Prior to the SPS procedure of tape formation, the samples were submitted to a series of cold working processes typical for the powder-in-tube technique. The tapes were compared with optimal doped bulk samples (having the same starting composition) and a pristine MgB2 tape. The morphology of the composite samples, the phase structure of both the core and the inner face of the metallic sheath shows the formation of a plethora of traces as a result of interaction between MgB2, additives, and the Fe sheath. Important critical parameters, like critical current density and the irreversibility field, show that there is a field and temperature range where the SiC and Te-added tapes display better critical parameters comparative to either pristine MgB2 tapes in the Fe sheath or SiC and Te doped MgB2 bulk samples.

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.

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.

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.

In melt-spun FePtB-based ribbons, the addition of Ag has been proven to decrease the temperature of phase transformation from the A1 fcc FePt phase to the hard magnetic tetragonal L1(0) phase. Alloys with 6 and 9 at.% Ag added to the initial FePtB have been synthesized by rapid solidification from the melt. The samples have been laser irradiated and submitted to nitriding procedure. This procedure has been proven beneficial for inducing complete transformation of A1 to L1(0) phase and a strong (001) texturing. Ag segregation combined to mechanisms of creation of vacancies and diffusion of N give rise to the formation of an intergranular disordered region and due to an improved interfacial coupling between FePt grains, enhanced coercivity and two-phase magnetic behavior is obtained.

Thin films of Bi2Sr2CaCu2O8 (Bi-2212) with the non-c-axis (117) orientation were grown by MOCVD on (110) LaAlO3 single crystal substrate. XRD theta - 2 theta scans show that films contain also (119) and (011) Bi-2212 impurity grains. We propose and report characterization of the non-c-axis films by XRD phi-psi scans. By this approach, the assumed theoretical film-substrate relationship of the (117) Bi-2212 grains is demonstrated experimentally. The result also confirms twinning in the span rooflike (117) Bi-2212 grains. The impurity (119) and (011) Bi-2212 grains are also rooflike and in-plane aligned according to film-substrate relation and AFM images so that the film can be considered in-plane epitaxial.