Publications

We demonstrate that under continuous single-beam excitation, one can generate an abnormal antiStokes Raman emission (AASRE) whose properties are similar to a coherent anti-Stokes Raman scattering. The effect has been observed in mesoscopic materials, which possess intrinsically nonlinear properties [lithium niobate (LiNbO3), bismuth germanium oxide (Bi12GeO20; BGO), bismuth silicon oxide (Bi12GeO20; BSO)], which have a nonzero electric susceptibility of the third order, chi((3)) not equal 0. Corroborated Raman and coherent backscattering studies demonstrate that the occurrence of both effects is conditioned by the existence of a mesoscopic morphology of the sample, which is able to ensure efficient transport of the light inside the sample through a multiple light scattering mechanism. In this context, both AASRE and coherent backscattering effects are because of the Anderson localization of the light. (C) 2014 Society of Photo-Optical Instrumentation Engineers (SPIE)

A kinetic analysis under non-isothermal conditions has been performed on europium-doped phosphate glasses with molar composition 20.42 Li2O-10.25 Al2O3-58.49 P2O5-7.23 BaO-1.44 La2O3-2.16 Eu2O3 and particle size 50 mu m. Differential scanning calorimetry measurements at four heating rates, from room temperature up to 900 degrees C using synthetic air have revealed that no significant mass change occurs during the heat treatment, as normally expected for glass samples. The step changes in heat flow signals are associated with the presence of three important effects: the first one, that occurs as a slope corresponds to the glass transition effect (T-g) is followed by two exothermic peaks, first of them more pronounced, associated with the first crystallization process (T-p1), while, the second one, lower in intensity corresponds to the second crystallization (T-p2) process. As expected, all peaks (T-g, T-p1 and T-p2) increase with the increasing of the heating rate. Both the activation energy of crystallization process and the crystallization mechanism were comparatively analyzed by two free-model estimations and using the formal theory of transformations for heterogeneous nucleation. (C) 2014 Elsevier Ltd and Techna Group S.r.l. All rights reserved.

We address theoretically the electronic transport through graphene quantum dots with the emphasis on the transmission phase. Analytical and numerical results are presented regarding the existence - or not - of a lapse of the transmittance phase (and, consequentially, a Fano zero in the transmittance) at the charge neutrality point. A simple universal criterium is found, the phase lapses being always present if the contact sites belong to the same sub-lattice. ((c) 2014 WILEY-VCH Verlag GmbH &Co. KGaA, Weinheim)

Tetragonal Sr2FeMoO6 powders were prepared by the sol gel and solid-state reaction methods. The structure, microstructure and magnetic characteristics of the double perovskite Sr2FeMoO6 in the form of as-prepared powders and classical sintered ceramics were analyzed and compared. Moreover, the magnetic properties of Sr2FeMoO6 ceramics obtained by sol gel and solid state reaction methods and sintered by the classical method were compared with those of Sr2FeMoO6 ceramics obtained by the same two methods, but sintered by the spark plasma sintering technique. The morphology of the powders obtained from the gel precursor and oxides mixture was characterized by homogeneity, as well as the grains shape and size. The powder prepared by the sol gel method was finer (particle average size of 0.6 mu m) than those obtained from oxides mixture (particle average size of 0.9 mu m). Sintered ceramics with tetragonal Sr2FeMoO6 phase were prepared from the two mentioned powders by classical sintering at 1200 degrees C, 2 h in 5%H-2/Ar. The pellets obtained from the gel powder exhibited higher magnetic characteristics than those derived from the oxides mixture. The saturation magnetization and the total magnetic moment of the samples prepared by the sol-gel method were M-sat=41.18 emu/g and mu(exp)/f.u.=3.26, respectively, while for the samples derived from the oxides mixture were M-sat=40.77 emu/g and mu(exp)/f.u=3.10. Also, Sr2FeMoO6 pellets sintered by the conventional method showed higher saturation magnetization values than those sintered by spark plasma sintering technique. (C) 2014 Elsevier Ltd and Techna Group S.r.l. All rights reserved.

Using surface-enhanced Raman scattering (SERS) and photoluminescence (PL) studies, new data concerning the electrochemical oxidation both of poly[(2,5-bisoctyloxy)-1,4-phenylene-vinylene] (BO-PPV) and the BO-PPV/HIPCO single-walled carbon nanotubes (SWNTs) composite are presented in this paper. The SERS studies performed at the excitation wavelengths of 752 nm and 532 nm of the BO-PPV/SWNTs composite that ensure the resonant excitation of the semiconductor and metallic nanotubes, respectively, reveal that the mixing of the two constituents results, on the one hand, in an isolation of semiconducting nanotubes from the bundles containing both metallic and semiconducting tubes and, on the other hand, in a functionalization of metallic SWNTs with BO-PPV. The isolation of semiconducting SWNTs is demonstrated by the narrowing of the G band and the change of the ratio between the intensities of the Raman lines situated in the low-frequency range that are assigned to the radial breathing vibrational modes. An additional isolation of the semiconducting nanotubes from the SWNTs bundles is reported when an electro-oxidation of the BO-PPV/SWNTs composite was performed in the potential range of (0; +2) V vs. Ag/AgCl. According to the Fourier transformed infra-red (FTIR) spectra and the SERS studies performed at an excitation wavelength of 1064 nm, the chemical interaction of BO-PPV with HIPCO SWNTs reveals a charge transfer between the two constituents that leads to the formation of BO-PPV covalently functionalized SWNTs. The BO-PPV luminescence quenching effect induced by the presence of SWNTs that consists of a change in the relative intensities of the three PL bands of the polymer peaked at 1.73 eV, 1.9 eV and 2.07 eV is due to the metallic tubes. The appearance of a new emission band at 2.32 eV was regularly observed when electrochemical oxidation of the BO-PPV/SWNTs composite was performed in the potential range of (0; +2) V. The PL band at 2.32 eV corresponds to ClO4- ions, which compensates the positive charges of BO-PPV generated during the electrochemical doping process. (C) 2014 Elsevier B.V. All rights reserved.