Temperature and high pressure effects on the structural features of catalytic nanocomposites oxides by Raman spectroscopy

被引:17
作者
da Silva, Antonio N. [1 ]
Pinto, Raffael C. F. [1 ]
Freire, Paulo T. C. [1 ]
Junior, Jose Alves L. [1 ]
Oliveira, Alcineia C. [2 ]
Filho, Josue M. [1 ]
机构
[1] Univ Fed Ceara, Dept Fis, Fortaleza, Ceara, Brazil
[2] Univ Fed Ceara, Dept Quim Anal & Fis Quim, Fortaleza, Ceara, Brazil
关键词
Raman spectroscopy; Phase transitions; Oxides; Nanostructures; Defects; Composite materials; INDUCED PHASE-TRANSITION; X-RAY-DIFFRACTION; NANOSTRUCTURED CERIA; MANGANESE OXIDES; FT-IR; SURFACE; TIO2; TRANSFORMATION; SCATTERING; ZIRCONIA;
D O I
10.1016/j.saa.2014.11.081
中图分类号
O433 [光谱学];
学科分类号
0703 ; 070302 ;
摘要
Structural characterizations of nanostructured oxides were studied by X-ray diffraction (XRD), Raman and infrared spectroscopy. The oxides catalysts namely, SnO2, ZrO2, CeO2, MnOx, Al2O3 and TiO2 were prepared by a nanocasting route and the effect of the temperature and pressure on the stability of the solids was evaluated. Raman spectra showed that ZrO2 and TiO2 exhibited phase transitions at moderate temperatures whereas CeO2, SnO2 and MnOx had an effective creation of defects in their structures upon annealing at elevated temperatures. The results suggested also that the effect of the temperature on the particles growth is related to the type of oxide. In this regard, phase transition by up to 600 degrees C accelerated the sintering of ZrO2 and CeO2 grains compared to TiO2, SnO2 and MnOx counterparts. Under hydrostatic pressures lower than 10 GPa, rutile TiO2 and tetragonal ZrO2 exhibited pressure induced phase transition whereas CeO2 and SnO2 were stable at pressures close to 15 GPa. The experiments revealed that the nanostructured SnO2 oxide exhibited stable performance at relatively high temperatures without phase transition or sintering, being suitable to be used as catalysts in the range of temperature and pressure studied. (C) 2014 Elsevier B.V. All rights reserved.
引用
收藏
页码:763 / 773
页数:11
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