3491
Carbon nanotubes from ethanol on Fe-Co/MgO catalysts and related interface phenomena
Lupu, D; Biris, AR; Baltog, I; Baibarac, M; Kuncser, V; Schinteie, G; Valeanu, M; Lefrant, S; Biris, AS; Misan, I; Filoti, G
MAR 2009, JOURNAL OF OPTOELECTRONICS AND ADVANCED MATERIALS, 11, 347
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Mossbauer spectroscopy studies of Fe-Co/MgO catalysts proved that a high dispersion degree of Fe may be achieved for catalysts containing Fe/Co in a ratio close to 1. During materials processing. the presence of hydrogen at high temperatures, even for short time, induced an increased particle size of the catalytic Fe. The evaluation of various iron species from their areas in the Mossbauer spectra revealed the dependence of the nanotube amount on (FeCo alloy + Fe2+) content in the catalyst, in good agreement with literature mechanisms. The Raman spectra show that carbon nanotubes synthesized from ethanol in argon flow on 4.5%Fe:4.5%Co/MgO are richer in low diameter (0.7-1.0nm) tubes than those obtained at low ethanol pressure, in agreement with the effects of hydrogen reported in literature. The close similarity with the Raman spectra of Aldrich double-walled carbon nanotubes and from literature, recommends the syntheses in argon flow as better conditions for double-walled carbon nanotube growth.
3492
Ceramic laser materials and the prospect for high power lasers
Lupei, V
MAR 2009, OPTICAL MATERIALS, 31, 706
DOI: 10.1016/j.optmat.2008.04.007
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The paper discusses the possibilities for enhancement of laser emission parameters and power scaling of Nd-doped transparent ceramic materials. It is shown that by a correlated approach that accounts for the properties of the laser material, pumping conditions and details of laser design, the direct diode laser pumping of these lasers into the emitting level F-4(3/2) enables additional power scaling in the range of 50-60% compared with the traditional 800 nm pumping in F-4(5/2).(.) (C) 2008 Elsevier B.V. All rights reserved.
3493
Composites containing confined n-octyl-cyanobiphenyl: Monomer and dimer species in the surface layer by in situ FTIR spectroscopy
Frunza, L; Frunza, S; Poterasu, M; Beica, T; Kosslick, H; Stoenescu, D
MAR 2009, SPECTROCHIMICA ACTA PART A-MOLECULAR AND BIOMOLECULAR SPECTROSCOPY, 72, 253
DOI: 10.1016/j.saa.2008.09.001
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Confinement of 4-n-octyl-4'-cyanobiphenyl (8CB) to nanoporous molecular sieves with hexagonal structure of cylindrical pores (4.6 nm diameter) is studied. Thermogravimetric investigations have indicated that the pores are completely filled. Several surface species inside the pores and onto the external surface of the grains were demonstrated by differential thermal analysis and by in situ infrared spectroscopy. Arguments are given that bulk-like monomer and dimer species along with hydrogen bonded ones might coexist in the so-called surface layer, but their population varies drastically as function of the temperature. In addition, chemical changes of the confined liquid crystal are quite possible inside these nanopores, at temperatures lower than for the bulk. (c) 2008 Published by Elsevier B.V.
3494
Upconversion emission of RE3+ in Sc2O3 ceramic under 800 nm pumping
Lupei, A; Lupei, V; Gheorghe, C; Ikesue, A; Osiac, E
MAR 2009, OPTICAL MATERIALS, 31, 749
DOI: 10.1016/j.optmat.2008.02.008
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The infrared (800 nm range) radiation conversion to visible in Er3+ doped or (Nd, Yb, Tm) co-doped Sc2O3 transparent ceramics was investigated. The green upconversion (H-2(11/2) -> S-4(3/2)) -> I-4(15/2) emission in Er - 3 (at low Er content) under pulsed pumping into (I-4(15/2) -> I-4(19/2)) absorption lines shows a competition between ESA (excited state absorption) (I-4(15/2) -> I-4(19/2)) + (I-4(19/2) -> H-2(9/2)) and ETU (energy transfer upconversion) (I-4(11/2) -> I-4(15/2)) +(I-4(11/2) -> F-4(7/2)) two-step processes, function on the excitation wavelength. The upconversion transfer rates were estimated. The features of the blue (1)G(4) -> H-3(6) Tm3+ upconversion emission in (Tm, Nd, Yb):Sc2O3 ceramic, under pumping at 808.3 nm were also analyzed. At this wavelength both Nd3+ and Tm3+ present ground state absorption. The data suggest that the population of Tm3+ (1)G(4) emitting level is achieved by the energy transfer processes Nd(F-4(3/2) -> I-4(11/2)) + Tm(H-3(4) -> (1)G(4)), or the chain Nd(F-4(3/2) -> I-4(19/2)) + Yb(F-2(1/2) -> F-2(5/2)) followed by the Yb(F-2(5/2) -> F-2(7/2)) + Tm(H-3(4) -> (1)G(4)), function on Yb3+ content. (C) 2008 Elsevier B.V. All rights reserved.
3495
All-self-assembled MgO nanorods and nanowires grown on Au-decorated MgO substrates by pulsed laser deposition
Crisan, A; Tanner, JL; Mikheenko, P; Abell, JS
MAR 2009, OPTOELECTRONICS AND ADVANCED MATERIALS-RAPID COMMUNICATIONS, 3, 235
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We report on the fabrication of MgO nanorods and nanowires by a novel, all-self-assembled method, using Pulsed Laser Deposition. The seeds for the formation of these one-dimensional nanostructures consisted of self-assembled gold nanodots. Gold was used due to its well-known catalytic effect. Dimensions and surface density of the Au nano-dots, investigated by Atomic Force Microscopy, depend on the deposition conditions and the number of laser pulses. Morphology of the MgO nanorods and nanowires was investigated by SEM, and was found to depend strongly on the deposition conditions and on the architecture of the Au nanodots on the decorated substrates.
3496
Artificial pinning centres in YBa2Cu3O7-delta thin films by Gd2Ba4CuWOy nanophase inclusions
Kechik, MMA; Mikheenko, P; Sarkar, A; Dang, VS; Babu, NH; Cardwell, DA; Abell, JS; Crisan, A
MAR 2009, SUPERCONDUCTOR SCIENCE & TECHNOLOGY, 22
DOI: 10.1088/0953-2048/22/3/034020
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Artificial pinning centres produced by Gd2Ba4CuWOy (2411W) nanophase inclusions in YBa2Cu3Oy (YBCO) thin films grown by pulsed laser deposition (PLD) using a YBCO target containing 1 mol% 2411W have been investigated. For comparison, YBCO thin films have been grown under the same conditions using a pure (commercial) YBCO target. The resulting films were characterized by AC susceptibility (superconducting transition) and SQUID magnetometry (critical current density, J(c)), and by x-ray diffraction (XRD), scanning electron microscopy (SEM), energy-dispersive x-ray (EDX) spectroscopy and atomic force microscopy (AFM) (structure, morphology and chemical composition). J(c) of the film grown from the composite target is practically the same as that measured for the reference sample at 5 K over the whole range of applied field up to 4.5 T. For temperatures higher than 50 K, however, the presence of the nano-inclusions leads to increased J(c). The relative enhancement in J(c) increases with further increase in temperature. J(c) of the film containing nanophase inclusions is between two and three times higher than that of the reference sample at 77.3 K and 1.5 T. This can be explained by considering the dimensions of nanophase inclusions compared with the temperature-dependent coherence length. Susceptibility measurements reveal that, apart from a large and sharp transition at about 91 K, there is a secondary, smaller and broader transition between 88 and 84 K in the YBCO film containing nanophase inclusions. This can be explained by substitutions of compatible atoms between YBCO and the 2411W phase (Gd with Y), which might also create additional pinning centres of delta T-c-type.
3497
Nonmonotonic flux flow in inhomogeneous superconductors above the percolation threshold
Sandu, V
FEB 1 2009, PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS, 469, 128
DOI: 10.1016/j.physc.2008.12.010
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Flux flow resistivity above critical temperature is analyzed based on the increased evidences that high temperature superconductors are intrinsically inhomogeneous, and local nonpercolating superconducting domains persist high above the critical temperature. It was found that above a certain field, the resistivity originated in the flow Of flux motion starts to decrease with increasing field, due to the predominance of the suppression of the superconducting droplets over the increase of vortex core density. (C) 2008 Elsevier B.V. All rights reserved.
3498
Fast and Simple Specimen Preparation for TEM Studies of Oxide Films Deposited on Silicon Wafers
Teodorescu, VS; Blanchin, MG
FEB 2009, MICROSCOPY AND MICROANALYSIS, 15, 19
DOI: 10.1017/S1431927609090011
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We present a fast and simple method to prepare specimen,, for transmission electron microscopy Studies of oxide thin films deposited oil silicon Substrates. The method consists of scratching the film surface using I pointed diamond tip, in a special manner. Small and thin fragments are then detached front the film and its substrate. Depending oil the scratching direction, the fragments call be used for plan-view or cross-section imaging. High-resolution images call be also obtained from thin edges of the film fragments. The method is demonstrated in the Case Of HfO2 sol-gel films deposited on [100] Si wafer substrates.
3499
Quantum well effect in bulk PbI2 crystals revealed by the anisotropy of photoluminescence and Raman spectra
Baltog, I; Baibarac, M; Lefrant, S
JAN 14 2009, JOURNAL OF PHYSICS-CONDENSED MATTER, 21
DOI: 10.1088/0953-8984/21/2/025507
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On subjecting a bulk 2H-PbI2 crystal to vacuum annealing at 500 K followed by a sudden cooling at liquid nitrogen temperature stacking faults are generated that separate distinct layers of nanometric thickness in which different numbers of I-Pb-I atomic layers are bundled together. Such structures, containing two, three, four, five etc I-Pb-I atomic layers, behave as quantum wells of different widths. The signature of such a transformation is given by a shift towards higher energies of the fundamental absorption edge, which is experimentally revealed by specific anisotropies in the photoluminescence and Raman spectra. The quantum confining effect is made visible by specific variations of a wide extra-excitonic band (G) at 2.06 eV that originates in the radiative recombination of carriers (electrons and holes), trapped on the surface defects. The excitation spectrum of the G band, with p polarized exciting light, reveals a fine structure comprised of narrow bands at 2.75, 2.64, 2.59 and 2.56 eV, which are associated with the PbI2 quantum wells formed from two, three, four and five I-Pb-I atomic layers of 0.7 nm thickness. Regardless of the polarization state of the laser exciting light of 514.5 nm (2.41 eV), which is close to the band gap energy of PbI2 (2.52 eV), the Raman scattering on bulk as-grown PbI2 crystals has the character of a resonant process. For p polarized exciting light, the Raman scattering process on vacuum annealed PbI2 becomes non-resonant. This originates from the quantum well structures generated inside the crystal, whose band gap energies are higher than the energy of the exciting light.
3500
Photonic molecular effects associated to the sputtering process in a glow discharge optical emission spectrometer
Surmeian, A; Groza, A; Diplasu, C; Ganciu, M; Teodorescu, CM; Tempez, A; Chapon, P
JAN 2009, OPTOELECTRONICS AND ADVANCED MATERIALS-RAPID COMMUNICATIONS, 3, 43
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Spectral emission of a Xenon discharge in the presence of NaCl powder is strongly modified and dominated by the XeCl excimer band at 308 nm. Materials introduced in gas electrical discharges interact with the reactive species produced in the plasma: electrons, ions and metastable atoms. In this paper, the influence of ions and metastable atoms of a capacitive RF Xenon discharge plasma (20W, 30MHz) 5 Torr on the structure of a NaCl powder introduced in the discharge has been investigated.