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1Thermal and structural properties of Nd2O3-doped calcium boroaluminate glasses显示文摘Nd^(3+) doped CaO-Al_2O-B_2O_3-CaF_2 glasses were prepared by conventional melt-quenching technique,and their structural and thermal properties were studied.The amorphous nature of these samples was confirmed by X-ray diffraction(XRD).The measured density showed an increase with Nd_2O_3 doping,at the expense of CaO.Raman spectra presented changes with addition of Nd_2O_3,which indicated that the network structure of the glasses studied presented various borate groups,such as tetraborates,metaborates,ortho-borates and pyroborates units.The N_4 values calculated from FTIR spectra revealed that incorporation of Nd_2O_3 into glass network converted the structural units from BO_4 to BO_3.From the analysis of DTA curves,we verified that Tg increased with the addition of Nd_2O_3;it was similar to the behavior caused by modifier oxides in the structure of borate glasses.Besides that,the calculated glass stability Tx–Tg for doped samples presented a decrease if compared to the undoped glass.Specific heat and thermal conductivity did not present significant changes with Nd_2O_3 concentration,up to 2.30 mol.%.The results of density,DTA,Raman and FTIR reinforced the idea that Nd_2O_3 acted as network modifier.J.D.M.Dias G.H.A.Melo T.A.Lodi J.O.Carvalho P.F.Facanha Filho M.J.Barboza A.Steimacher F.Pedrochi 2016Journal of Rare Earths2016,34,5:6
2Thermal stability and spectroscopic properties of Ho^(3+) doped tellurite-borate glasses显示文摘Ho3+ ions doped tellurite-borate glass samples with varying compositions were prepared. The compositional dependence on phenomenological Judd-Ofelt parameters was compared in different kinds of rare earth ions doped tellurite-borate glasses. Two methods were used to obtain radiative transition probability of 5I7 level with the aim of assuring the fitting quality. The integral absorption cross-sections and line shapes corresponding to 5I8→5G6 and 5I8→5I7 transition of Ho3+ ions were investigated in tellurite-borate glasses. The obtained data indicated that the integral absorption cross-sections corresponding to 5I8→5G6 transition of Ho3+ ions mainly depended on phenomenological Judd-Ofelt parameter, ?2, because 5I8→5G6 transition belonged to hypersensitive transitions, which led to a larger ?2 value. The change of line shapes of absorption spectra corresponding to 5I8→5G6 and 5I8→5I7 transitions of Ho3+ ions came from the lower energy regions, which could be attributed to the changed distribution of Stark levels and thermal population.杨艳民 刘延洲 蔡培庆 Ramzi Maalej Hyo Jin Seo 2015Journal of Rare Earths2015,33,9:1
3Preparation by chemical co-precipitation, spectral and electrical characteristics of neodymium orthophosphate nanoparticles显示文摘Nanoparticles of neodymium orthophosphate(Nd PO4) were prepared through a facile wet co-precipitation technique. The X-ray diffraction(XRD) studies revealed the material belonging to monoclinic monazite phase with crystallite size of 30.8 nm. Scanning electron microscopic studies showed that the material was composed of a large number of agglomerated spherical particles having grain size of 92 nm. Thermogravimetric analysis suggested that the structural phase transition was seen above 800 °C. The spectroscopic investigations were carried out using Fourier transform infrared spectroscopy(FTIR). UV-VIS-NIR absorption spectrophotometer showed various transitions from the ground state 4I9/2 to various excited states within the 4f shell and the optical band gap came out to be 3.3 e V. The dielectric constant(ε′), dielectric loss(tan δ) and ac conductivity ln(σac) were measured in the frequency range of 5 k Hz to 1 MHz and in the temperature range of 40 to 500 °C. The dielectric measurement suggested that there was a shift in the value of transition temperature(Tc), thereby indicating relaxor behaviour of the material. The activation energy value decreased with increase in frequency, thereby suggesting the role of mixed ionic-polaronic conductivity.Seema Verma K.K.Bamzai 2015Journal of Rare Earths2015,33,5:0
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