4631
Metastable phases and crystallization products in nanocrystalline FINEMET-type alloys with RE addition
Crisan, AD; LeBreton, JM; Crisan, O; Filoti, G
SEP 2003, JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS, 5, 711
Show abstract
The melt spun nanocrystalline alloys such as Fe73.5Cu1Nb3Si13.5B9 (FINEMET) have attracted great deal of interest in recent years due to their excellent soft magnetic properties mostly related to the exchange coupling between nanograins, through the amorphous matrix. The microstructural evolution of both nanocrystalline and amorphous residual phases during annealing of the ribbons give rise to crystallization products that determine the expected magnetic properties for specific applications. Upon addition of the rare earth (RE), the evolution of the crystalline phases which emerge from metastable precursors during annealing is investigated. It is expected that the RE presence should strongly modify both the phase structure via new ternary metastable precursors and the magnetic properties of the ribbons by inducing enhanced exchange correlation due to novel ternary crystalline phases.
4632
Numerical simulations of the backscattering from a crystalline lattice
Ciobanu, A; Babin, V; Nicolae, DN; Talianu, C; Morosanu, C
SEP 2003, JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS, 5, 660
Show abstract
The backscattering of 100, 300, and 500 eV Ar atoms from the {100} and {110} planes of a Al crystalline target is investigated with a computer code based on the Molecular Dynamics(MD) method. The interactions between particles are described by a screened Coulomb type potential. The angular (both azimuthal and radial) distribution of the backscattered particles together with the distribution of the energy and of the energy loss of scattered particles are calculated using the Lindhard-Scharff parameterization. The azimuthal distribution shows high peaks for 300 and 500 eV incident energies and a cvasi-continuum for 100 eV incident energy in the case of {100} plane, and a single peak for the {110} plane. The radial. distribution of backscattered particles evidences the symmetry properties of the crystal. The relative energy loss decrease when increasing incident energy, and is compatible with the backscattered energy distribution. The results do not agree with the Binary Collision Approximation(BCA).
4633
Growth and properties of Pb(ZrxTi1-x)O-3 step graded-structures
Boerasu, I; Pintilie, L; Pereira, M; Gomes, MJM; Vilarinho, PM
SEP 2003, JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS, 5, 775
Show abstract
Pb(Zr-x Ti1-x)O-3 (x = 55, 65, 92), PZT step graded-structure have been deposited by sol-gel technique on Pt-coated Si. Up-graded and down-graded structures has been obtained by changing the Zr/Ti ratio in steps a long to the film thickness. Up means that the ratio was increased from the bottom to the top while down means it was decreased. The properties of these films were investigated and compared with those of conventional films with homogeneous composition. It was found that the properties of up and down graded structures are completely different. Up-graded films have better ferroelectric properties than the downgraded ones. Pyroelectric signal could be detected also on as-grown up-graded films, in accordance with the structural results that show a strong (100) orientation in this case, The coercive field of the up-graded film is lower than the values obtained in case of homogeneous films with the same Zr/Ti ratios like those used in the graded structures.
4634
The role of TiO in the perovskite nucleation and (111) orientation selection in sol-gel PZT layers
Vasiliu, F; Norga, GJ; Fe, L; Wounters, D; Van der Biest, D
SEP 2003, JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS, 5, 785
Show abstract
We have proposed a lattice matching mechanism for the selection of (111) PZT orientation, based on the! experimental evidence of the formation of cubic TiO on the Pt electrode surface in the earlier stages of thermal processing of PZT layers Thus, a fitting of TiO with Pt and, consequently of PZT (Ti-rich) with TiO (orientation relationship:TiO (111)//Pt(111) and respectively PZT(111)//TiO(111)) has been evaluated. Similar mismatch degree values were obtained comparatively with the classical cases of intermetallic layer "templates" (for example PtxPb, Pt3Ti, etc). The very good lattice matching supports the proposed mechanism, consisting in the formation of cubic TiO on Pt and, later, of the nucleation and growth of PZT (tetragonal) of cubic TiO, where is formed. In comparison with the case of TiO2(rutile) matching, previously proposed by other groups,having larger mismatch values,the cube-to-cube orientation relationship could explain the selection of (111) orientation as a major one in some specific conditions affected by some parameters especially related to solution chemistry and thermal processing steps.
4635
Microstructure and mechanical properties of hydroxyapatite thin films grown by RF magnetron sputtering
Nelea, V; Morosanu, C; Iliescu, M; Mihailescu, IN
AUG 22 2003, SURFACE & COATINGS TECHNOLOGY, 173, 322
DOI: 10.1016/S0257-8972(03)00729-1
Show abstract
Hydroxyapatite (HA) thin films for applications in bone prosthesis fabrication were obtained by the radio-frequency magnetron sputtering technique. The depositions were performed from pure HA targets on Si and Ti-5AI-2.5Fe alloy substrates. In some experiments a buffer layer of TiN was introduced by pulsed laser deposition before HA coating. The films were deposited in low-pressure argon or Ar-O-2 mixtures at substrate temperatures ranging from 70 to 550 degreesC. We observed that the films grown at temperatures below 300 degreesC were prevalently amorphous and contain a small amount of crystalline material. The initial crystalline structure of the target is reconstructed after 1 h films annealing at 550 degreesC in ambient air. Both the films directly deposited at 550 degreesC and the ones obtained at room temperature and after that annealed at this temperature-mostly contain the HA phase and exhibit good mechanical characteristics. Weaker peaks of CaO secondary phase are visible in the X-ray diffraction patterns of the films directly grown at 550 degreesC. Traces of TiO2 were detected at the interface with the metallic substrate in case of structures grown without the TiN interlayer. All films were smooth, with an average surface roughness of 50 nm. The films grown on TiN interlayer are harder, have higher elasticity modulus values and an increased mechanical resistance at the indenter penetration. (C) 2003 Elsevier Science B.V. All rights reserved.
4636
Morphology, structure and optical properties of sol-gel ITO thin films
Stoica, TF; Teodorescu, VS; Blanchin, MG; Stoica, TA; Gartner, M; Losurdo, M; Zaharescu, M
AUG 15 2003, MATERIALS SCIENCE AND ENGINEERING B-SOLID STATE MATERIALS FOR ADVANCED TECHNOLOGY, 101, 226
DOI: 10.1016/S0921-5107(02)00667-0
Show abstract
The alkoxidic route and the spinning deposition were used to prepare monolayer sol-gel indium tin oxide (ITO) films. The morphology and crystalline structure were investigated by cross-section transmission electron microscopy (XTEM) and atomic force microscopy (AFM). The ITO sol-gel mono-layer contains three regions of different porosities. The basic crystalline structure is that of the In2O3 lattice. The optical properties have been studied by optical transmission and spectroscopic ellipsometry. (C) 2003 Elsevier Science B.V. All rights reserved.
4637
Effect of substitutions on the hyperfine magnetic field in Nd-based intermetallics
Sorescu, M; Valeanu, M; Diamandescu, L
AUG 2003, INTERMETALLICS, 11, 754
DOI: 10.1016/S0966-9795(03)00076-1
Show abstract
The present work is focused on several 2:17 intermetallic compounds, namely Nd2Fe15Si2, Nd2Fe15Al2, Nd2Fe15SiAl and Nd2Fe15SiMn as well as several 1:12 intermetallic compounds, such as NdFe10Si2, NdFe10Al2, NdFe10SiAl and NdFe10MnAl. The substitutional effect on their magnetic properties is studied by Mossbauer spectroscopy using hyperfine magnetic field distributions. The single-phase structure of both classes of intermetallics was supported by X-ray diffraction (XRD) measurements. (C) 2003 Elsevier Ltd. All rights reserved.
4638
Propane ammoxidation catalyst based on vanadium-aluminum oxynitride
Silvy, RP; Florea, M; Blangenois, N; Grange, P
AUG 2003
DOI: 10.1002/aic.690490830
4639
Exciton-phonon interaction in semiconductors with intermediate polar coupling
Schafer, W; Gartner, P; Jahnke, F
AUG 2003, PHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICS, 238, 555
DOI: 10.1002/pssb.200303188
Show abstract
The importance of vertex corrections in the description of the absorption spectra in semiconductors is discussed. These corrections are responsible for the excitonic correlation of the phonon-scattered carriers and it is shown that these correlations are essential for the description of excitonic sidebands in the case of intermediate coupling. Different approximation schemes are compared in numerical examples.
4640
Vortex melting line and anisotropy of high-pressure-synthesized TlBa2Ca2Cu3O10-y high-temperature superconductor from third-harmonic susceptibility studies
Crisan, A; Iyo, A; Tanaka, Y
JUL 21 2003, APPLIED PHYSICS LETTERS, 83, 508
DOI: 10.1063/1.1593824
Show abstract
The fundamental and third-harmonic susceptibility response of YBa2Cu3O7-delta (YBCO) and TlBa2Ca2Cu3O10-y (Tl:1223) high-critical temperature (T-c) superconductors with preferentially oriented crystallites has been measured in various magnetic fields up to 14 T, and with very low ac field amplitude, to probe the melting transition of the vortex matter. This method does not require large single crystals, being therefore suitable for high-T-c superconductors with small crystallites, prepared with high-pressure synthesis techniques. We determine experimentally the melting line of vortices and the anisotropy factor in high-pressure-grown Tl:1223 with a high T-c of 133.5 K. Results from similar measurements on YBCO with preferentially oriented grains are consistent with both commonly accepted models of the melting line and values of the anisotropy factor, supporting the validity of our approach. (C) 2003 American Institute of Physics.