Síntese e caracterização óptica de vidros da família TeO2 -B2O3 -(Bi2O3 ou WO3)
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Data
2018-08-30
Autores
Leandro, Silvana Castro
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Universidade Estadual Paulista (Unesp)
Resumo
Vidros a base de óxidos de metais pesados (TeO2, WO3, Bi2O3) apresentam alto índice de refração, altos valores de não-linearidade óptica e alta constante dielétrica. Essas propriedades físicas possibilitam diversas aplicações, como, por exemplo, para comutação ultrarrápida em dispositivos ópticos e, exibem, quando dopados com terras raras, importantes propriedades de luminescência [1]. Vidros dos sistemas ternários xTeO2 – yB2O3 – zWO3 e xTeO2 – yB2O3 – kBi2O3 foram preparados pelo método “melt-quenching” com x de 70 a 45%mol, y de 40 a 10%mol, z de 30 a 15%mol e k com variação de 20 a 10%mol. Introduzimos o óxido de Boro para dar maior viscosidade ao material e aumentar a estabilidade térmica. Foram obtidas amostras homogêneas e transparentes para as seguintes composições: 70TeO2–10B2O3–20WO3, 70TeO2–20B2O3–10Bi2O3 e 55TeO2 –30B2O3–15Bi2O3. Dados de espectroscopia de IR revelaram que a rede dos vidros consiste basicamente das seguintes unidades estruturais: [TeO4], [WO4], [WO6], [BO4], [BO3] e Te-O-W para o sistema TeO2 – B2O3 – WO3 e de [TeO4], [BiO3], [BiO6], [BO4], [BO3] para o sistema TeO2 – B2O3 – Bi2O3. Medidas de absorção óptica das amostras foram realizadas antes e após a exposição a irradiação gama em doses de 10Gy, 1kGy, 10kGy e 50kGy e forneceram valores das bordas de absorção no intervalo de 378 a 449 nm. Obtiveram-se índices de refração da ordem de n > 2 em 633 nm através do equipamento Interferômetro de Michelson e método do ângulo de Brewster. As energias do gap óptico (Eg) obtidas desses vidros são da ordem de ≈ 2 a 3 eV.
Glasses based on heavy metal oxides (TeO2, WO3, Bi2O3) have high refractive index, high values of optical nonlinearity and high dielectric constant. These physical properties enable a variety of applications, such as for ultrafast switching in optical devices and, when doped with rare earths, exhibit important luminescence [1]. Glasses in the ternary systems xTeO2–yB2O3–zWO3 and xTeO2–yB2O3–kBi2O3 were prepared from melt quenching method with x from 70 to 45 mol%, y from 40 to 10 mol%, z from 30 to 15 mol% and k with variation from 20 to 10 mol%. We introduce the Boron oxide to give a higher viscosity to the material, ie, higher thermal stability. Homogeneous and transparent samples were obtained for the following compositions: 70TeO2–10B2O3–20WO3, 70TeO2–20B2O3–10Bi2O3 and 55TeO2 –30B2O3–15Bi2O3. FTIR spectroscopy data revealed that the glass basically consists of the following structural units: [TeO4], [WO4], [WO6], [BO4], [BO3] and Te-O-W to the system TeO2–B2O3–WO3 and [TeO4], [BiO3], [BiO6], [BO4], [BO3] to the system TeO2–B2O3–Bi2O3. Optical absorption measurements of the samples were performed before and after exposure to gamma irradiation at doses of 10Gy, 1kGy, 10kGy and 50kGy and provided absorption edge values in the range of 378 to 449 nm. Were obtained refractive index of the order of n> 2 at 633 nm through the equipment Michelson´s Interferometer and Brewster's angle method. The optical gap energies obtained from these glasses are of the order of ≈ 2 to 3 eV.
Glasses based on heavy metal oxides (TeO2, WO3, Bi2O3) have high refractive index, high values of optical nonlinearity and high dielectric constant. These physical properties enable a variety of applications, such as for ultrafast switching in optical devices and, when doped with rare earths, exhibit important luminescence [1]. Glasses in the ternary systems xTeO2–yB2O3–zWO3 and xTeO2–yB2O3–kBi2O3 were prepared from melt quenching method with x from 70 to 45 mol%, y from 40 to 10 mol%, z from 30 to 15 mol% and k with variation from 20 to 10 mol%. We introduce the Boron oxide to give a higher viscosity to the material, ie, higher thermal stability. Homogeneous and transparent samples were obtained for the following compositions: 70TeO2–10B2O3–20WO3, 70TeO2–20B2O3–10Bi2O3 and 55TeO2 –30B2O3–15Bi2O3. FTIR spectroscopy data revealed that the glass basically consists of the following structural units: [TeO4], [WO4], [WO6], [BO4], [BO3] and Te-O-W to the system TeO2–B2O3–WO3 and [TeO4], [BiO3], [BiO6], [BO4], [BO3] to the system TeO2–B2O3–Bi2O3. Optical absorption measurements of the samples were performed before and after exposure to gamma irradiation at doses of 10Gy, 1kGy, 10kGy and 50kGy and provided absorption edge values in the range of 378 to 449 nm. Were obtained refractive index of the order of n> 2 at 633 nm through the equipment Michelson´s Interferometer and Brewster's angle method. The optical gap energies obtained from these glasses are of the order of ≈ 2 to 3 eV.
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Palavras-chave
Vidros teluretos, Interferômetro de Michelson, Absorção óptica, Irradiação gama, Tellurite glasses, Michelson´s interferometer, Optical absorption, Gamma irradiation