Publications

5,974 articles found

4981

Intermediate frustration in [Fe3O(CH3COO)(6)(H2O)(3)] NO3 center dot 4(H2O) trinuclear cluster

Filoti, G; Bartolome, J; Dickson, DPE; Rillo, C; Prisecaru, I; Jovmir, T; Kuncser, V; Turta, C

MAY 1999, JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, 196, 563

DOI: 10.1016/S0304-8853(98)00825-7

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The frustration of the trinuclear clusters with antiferromagnetic intracluster interaction was investigated at low temperature and in applied magnetic field, by Mossbauer, susceptibility and magnetisation measurements. The spin configuration and the electronic state are described as a function of the temperature and the intensity of the applied field. The values of the exchange integrals are provided. (C) 1999 Elsevier Science B.V. All rights reserved.

4982

Studies by SERS spectroscopy of the structural properties of conducting polymers and carbon nanotubes

Lefrant, S; Baltog, I; de la Chapelle, ML; Baibarac, M; Louarn, G; Journet, C; Bernier, P

MAY 1999, SYNTHETIC METALS, 101, 187

DOI: 10.1016/S0379-6779(98)00307-5

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After being dispersed in liquid solvents (Ethanol, CHCl3), conducting polymers and singlewalled nanotubes have been deposited on ruguous substrats (Au, Ag, Cu). With FT Raman technique (laser excitation : 1064 nm), we have obtained SERS signal of both conductiong polymers and singlewalled nanotubes. The Raman signals change with substrat and/or solvent, which could be correlated with the size of clusters formed at the surface and then to the deposition mechanism. The main advantage of the >SERS technique will be emphasized in terms of enhancement as a powerful technique to study nanoparticles.

4983

Structural and magnetic properties of magnetoresistive Cu-Co-Fe ribbons

Crisan, O; Le Breton, JM; Jianu, A; Maignan, A; Nogues, M; Teillet, J; Filoti, G

MAY 1999, JOURNAL OF MAGNETISM AND MAGNETIC MATERIALS, 196, 469

DOI: 10.1016/S0304-8853(98)00822-1

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Melt-spun Cu80Co10Fe10 ribbons are shown to exhibit a nanogranular structure with magnetic alpha-Fe(Co) grains segregated from the Cu-rich matrix after appropriate annealing. The Cu matrix purification as well as the magnetic properties of the alpha-Fe(Co) grains existing in a range of sizes are studied using X-ray diffraction, Mossbauer spectrometry and magnetic measurements. There is an optimum annealing for obtaining a high magnetoresistive effect. (C) 1999 Elsevier Science B.V. All rights reserved.

4984

Radiation damage on p-type silicon detectors

Pirollo, S; Biggeri, U; Borchi, E; Bruzzi, M; Catacchini, E; Lazanu, S; Li, Z; Sciortino, S

APR 21 1999, NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION A-ACCELERATORS SPECTROMETERS DETECTORS AND ASSOCIATED EQUIPMENT, 426, 130

DOI: 10.1016/S0168-9002(98)01480-6

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Two sets of p-type silicon thigh resistivity bulk and low resistivity epitaxial) samples and one set of n(+)-p junctions have been irradiated with fast neutrons up to 8 x 10(13) cm(-2). I-V and C-V characteristics as well as Thermally Stimulated Currents (TSC) and Hall Effect (HE) analyses have been performed on the irradiated samples and diodes in view to determine the radiation-induced damage and the change in the electrical properties. A change in the effective carrier concentration and in the leakage current after irradiation similar to the one found for p(+)-n detectors has been observed in p-type diodes. An increase with the fluence of the resistivity and Hall coefficient was measured at room temperature both for the low and high resistivity sets. This evidence has been explained in terms of a two-level model taking into account a linear increase in concentration with the fluence of the main radiation-induced defects observed with TSC, probably related to divacancy and carbon-oxygen complex. (C) 1999 Elsevier Science B.V. All rights reserved.

4985

Multilayer structures deposited by laser ablation

Dinescu, M; Stanciu, C; Ghica, D; Dinu, R; Sandu, V; Nastase, N; Balucani, M; Bondarenko, V; Frachina, L; Lamedica, G; Ferrari, A

APR 20 1999, SENSORS AND ACTUATORS A-PHYSICAL, 74, 30

DOI: 10.1016/S0924-4247(98)00331-8

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TiN/Si structures were deposited on Si wafers by pulsed laser deposition technique. The highly conductive TiN films were grown on heated (100) Si substrates by laser ablation of a high purity Ti target in nitrogen reactive atmosphere. Subsequently, the Si layer was deposited by laser ablation of a Si target in vacuum (down to 10(-6) mbar) or in low pressure inert gas. The nitrogen gas pressure and the substrate temperature were found to strongly influence the TiN film structure and orientation. The degree of crystallinity of the Si layer grown on the TiN film was found to depend on Si/TiN collector temperature. Values below 550 degrees C (the threshold of TiN oxidation activation) were used in the experiments. Techniques as X-ray Diffraction (XRD), Fourier Transform Infrared Spectroscopy (FTIR), High Resolution Transmission Electron Microscopy (HRTEM), Scanning Force Microscopy (SFM) have been used to characterize the deposited structures. The TiN/Si structure rectifying properties were tested. The obtained Si/TiN/Si structure could be suitable for the building of Permeable Base Transistor (PBT, vertical MESFET) devices. (C) 1999 Elsevier Science S.A. All rights reserved.

4986

Pulsed laser deposition of multilayer TiN/Pb(ZrxTi1-x)O-3 for piezoelectric microdevices

Verardi, P; Dinescu, M; Craciun, F; Dinu, R; Sandu, V; Tapfer, L; Cappello, A

APR 20 1999, SENSORS AND ACTUATORS A-PHYSICAL, 74, 44

DOI: 10.1016/S0924-4247(98)00342-2

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Multilayer Pb(ZrTi)O-3 (PZT)/TiN/Si structures were grown by two subsequent laser ablation processes in reactive atmosphere. First, a fee-oriented TiN film was deposited by laser ablation of a Ti target in high-purity nitrogen reactive gas. Subsequently, a crystalline, piezoelectric PZT film was grown by reactive ablation of a PZT target in oxygen atmosphere. Both deposition processes were conducted at quite low Si(100) substrate temperature: 350 degrees C for TiN and 370 degrees C for PZT, in the same experimental setup (Nd-YAG laser, lambda = 1060 nm, energy/pulse 0.3 J, t(FWHM) = 10 ns). TiN film properties were analyzed by XRD and electric measurements. After the deposition of the PZT layer, the obtained structure was first characterized by XRD, SEM and SIMS techniques. Testing measurements performed after the deposition by thermal evaporation of an Al layer as top electrode on the PZT/TiN/Si structure confirm that they can be used as sensor transducer element. The TiN (as high conductive nitride) layer replaces the former Au layer used as bottom electrode. In this way, the Au diffusion inside the Si substrate, as well as in the deposited layer, is avoided, as could be observed from a comparative study of the SIMS spectra recorded for PZT/TiN/Si and PZT/Au/Si configurations. (C) 1999 Elsevier Science S.A. All rights reserved.

4987

The crucial role of particle morphology in the magnetic properties of haematite

Sorescu, M; Brand, RA; Mihaila-Tarabasanu, D; Diamandescu, L

APR 15 1999, JOURNAL OF APPLIED PHYSICS, 85, 5548

DOI: 10.1063/1.369890

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Haematite particles of four different morphologies (polyhedral, platelike, needlelike and disk shaped) were synthesized by the hydrothermal method. The morphology and average particle diameter (1.4, 7.4, 0.2, and 0.12 mm, respectively) were determined by transmission electron microscopy combined with electron diffraction. The haematite samples were studied by transmission Mossbauer spectroscopy in the temperature range 4.2-300 K. In all cases, a weak ferromagnetic (WF) phase was present above the Morin temperature of 230 K and found to coexist with an antiferromagnetic (AF) phase below this temperature. However, the populations of the two phases at 230 K were demonstrated to depend on the morphology of the particles. Moreover, the WF and AF phases exhibit a different dependence of the magnetic texture on temperature and particle morphology. (C) 1999 American Institute of Physics. [S0021-8979(99)66908-0].

4989

Growth of pure and doped Rb2ZnCl4 and K2ZnCl4 single crystals by Czochralski technique

Stefan, M; Nistor, SV; Mateescu, DC; Abakumov, AM

APR 1999, JOURNAL OF CRYSTAL GROWTH, 200, 154

DOI: 10.1016/S0022-0248(98)01247-0

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High-quality single crystals of Rb2ZnCl4 and K2ZnCl4, pure or doped with Cu, Mn, Cd, Tl, Sn, Pb and In cations, were grown by Czochralski technique in argon atmosphere, using an experimental setup that allows direct visual access to the whole growth zone. Slowly cooled crystals exhibit excellent cleavage properties. Fastly cooled crystals do cleave poorly. As shown by X-ray diffraction studies, such K2ZnCl4 samples exhibit inclusions of the high-temperature Pmcn phase with lattice parameters a = 7.263(2) Angstrom, b = 12.562(2) Angstrom and c = 8.960(4) Angstrom in the P2(1) cn room temperature stable phase. ESR and optical spectroscopy studies revealed the localization and valence state of the cation dopants. (C) 1999 Elsevier Science B.V. All rights reserved.

4990

Physico-chemical properties and X-ray study of trinuclear carboxylate [Fe3O(CH3COO)(6)(H2O)(3)](2)[PtCl6]center dot 8H(2)O

Turta, C; Shova, S; Meriacre, V; Cadelnic, I; Gdaniec, M; Simonov, YA; Filoti, G

APR 1999, POLISH JOURNAL OF CHEMISTRY, 73, 618

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Trinuclear carboxylate compound [Fe3O(CH3COO)(6)(H2O)(3)](2)[PtCl6].8H(2)O has been studied by Mossbauer spectroscopy, magnetochemistry, thermal analysis and X-ray crystallography. Crystal data: monoclinic, space group P2(1)/n a = 10.505(2), b = 14.278(3), c = 19.885(4) Angstrom, beta = 96.00(3)degrees and Z = 2. The final R-value is 0.027 for 4606 reflections with I greater than or equal to 2 sigma(I). The crystal consists of the complex [Fe3O(CH3COO)(6)(H2O)(3)](+) cations, centrosymmetric [PtCl6](2-) anions and water molecules. The [Fe3O(CH3COO)(6)(H2O)(3)](+) cation has the typical structure of a trinuclear iron(III) compound with mu(3)-O bridge. All crystal components are connected via a system of hydrogen bonds into a 3D network. Mossbauer spectrum displays at room temperature a single quadrupole doublet with an isomer shift of 0.70 mm/s and quadrupole splitting of 0.48 mm/s, consistent with high-spin Fe(III). mu(eff) per Fe atom (3.25 mu(B) at 293 K and 2.23 mu(B) at 120 K), indicate the antiferromagnetic coupling between the paramagnetic iron ions with J = -31 cm(-1).