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Preparation and Optical Properties of Er~(3+) -Doped Gadolinium Borosilicate Glasses

机译:掺Er〜(3+)硼硅酸Glasses玻璃的制备及光学性能

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Er~(3+) -doped Gd_2O_3 -SiO_2-B_2O_3 -Na_2O glasses were prepared, and formation range of glass of Gd_2 O_3-SiO_2-B_2O_3 system was experimentally obtained. It is found that the glass phase can be formed only when the content of SiO_2 is 0~50% (molar fraction), Gd_2O_3 is 0~30% (molar fraction) and B_2O_3 is above 20% (molar fraction) in this glass system. The glass can also be obtained but becomes translucent at the contents of 60% (molar fraction) SiO_2 and 30% Gd_2O_3, or at the contents of 60% (molar fraction) SiO_2 and 30% (molar fraction) B_2O_3. There is no glass phase formed in other glass components. Glass forming ability for Gd_2O_3 content of 10% , was characterized by the value of β, the parameter of crystallization tendency, which is 0.32 ~ 1.76, obtained from the differential thermal analysis. The absorption and emission cross section, the J-O parameters Ωt_(2,4,6) and radiative transition probabilities were calculated by using the theory of McCumber and Judd-Ofelt. The emission properties at 1.5 μm of the samples are discussed with the product of full width at half maximum and stimulated emission cross section. It can be seen that the value of the FWHM x σ_e~(peak) product in the prepared glass is more than those of germanate, silicate and phosphate glasses. Furthermore , the maximum value of the product among these glasses reported in this work is close to that of oxyfluoride silicate glass. Therefore, the Er~(3+)-doped gadolinium borosilicate glass in this paper is a candidate for broadband erbium doped fiber amplifiers.
机译:制备了掺Er〜(3+)的Gd_2O_3 -SiO_2-B_2O_3-Na_2O玻璃,并通过实验获得了Gd_2O_3-SiO_2-B_2O_3体系玻璃的形成范围。发现该玻璃体系中只有当SiO_2的含量为0〜50%(摩尔分数),Gd_2O_3为0〜30%(摩尔分数),B_2O_3大于20%(摩尔分数)时,才能形成玻璃相。 。也可以得到玻璃,但是在含量为60%(摩尔分数)的SiO_2和30%Gd_2O_3或在含量为60%(摩尔分数)的SiO_2和30%(摩尔分数)的B_2O_3时是半透明的。在其他玻璃组件中没有形成玻璃相。 Gd_2O_3含量为10%时的玻璃形成能力,由差热分析得到的β值,即结晶趋势参数0.32〜1.76表征。吸收和发射截面,J-O参数Ωt_(2,4,6)和辐射跃迁概率是根据McCumber和Judd-Ofelt理论计算的。讨论了样品在1.5μm处的发射特性,其中半峰全宽和受激发射截面为乘积。可以看出,所制备的玻璃中FWHM xσ_e_(peak)乘积的值大于锗酸盐,硅酸盐和磷酸盐玻璃的值。此外,在这项工作中报道的这些玻璃中产品的最大值接近于氟氧化硅酸盐玻璃的最大值。因此,本文中掺Er(3+)的g硼硅酸盐玻璃是宽带掺do光纤放大器的候选材料。

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