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A novel method for uniform dispersion of the rare earth ions in SiO2 glass using zeolite X

机译:X型沸石使稀土离子均匀分散在SiO2玻璃中的新方法

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摘要

A novel method for uniform dispersion of the rare earth ions in SiO2 glass is presented. Nd doped SiO2 laser glass has been made by aluminum co-doping to avoid quenching due to Nd clustering. Previous works with aluminum co-doping were passive methods because uniform dispersion of the rare earth ions in SiO2 glass depended only on aluminum co-doping effect. Concentration quenching of Nd laser glass is explained by cross-relaxation process and depends on Nd-Nd distance in the glass. The shorter the Nd-Nd distance the stronger is quenching, so the distance should be greater than some minimum. Homogeneous rare earth doped SiO2 glass is achieved by a modified sol-gel method using zeolite X. Zeolite X (Na-86[(AlO2)(86). (SiO2)(106)] . 264H(2)O, faujasite-type structure) is a suitable material because Nd ions are selectively exchanged at the D6R segment structure in zeolite X, and the distance between Nd ions in the D6R is 0.88 nm. This distance is three times larger than the critical range of cross-relaxation process which causes quenching. If the Nd-Nd distance is kept at 0.88 nm, the ratio of cross-relaxation probability to radiative decay probability will be 0.23%. Quantum yield is an adequate quantity for confirming uniform dispersion of the rare earth ions in Nd doped laser media. For a newly prepared Nd doped SiO2 glass using zeolite X, quantum yield increased to 50 +/- 3.4% at 1.0 wt%, while an ordinary produced one was 7 +/- 0.5%. (C) 1997 Elsevier Science B.V.
机译:提出了一种将稀土离子均匀分散在SiO2玻璃中的新方法。 Nd掺杂的SiO2激光玻璃已经通过铝共掺杂制成,以避免由于Nd团簇而淬火。以前的铝共掺杂工作是被动方法,因为稀土离子在SiO2玻璃中的均匀分散仅取决于铝共掺杂效应。 Nd激光玻璃的浓度淬火通过交叉弛豫过程来解释,并且取决于玻璃中Nd-Nd的距离。 Nd-Nd距离越短,淬灭越强,因此该距离应大于一些最小值。均质稀土掺杂的SiO2玻璃是通过改良的溶胶-凝胶法使用沸石X.沸石X(Na-86 [(AlO2)(86)。(SiO2)(106)]。264H(2)O,八面沸石型由于Nd离子在沸石X中的D6R链段结构上选择性地交换,并且D6R中Nd离子之间的距离为0.88nm,因此是合适的材料。该距离比引起淬火的交叉松弛过程的临界范围大三倍。如果Nd-Nd距离保持在0.88nm,则交叉弛豫几率与辐射衰减几率之比将为0.23%。量子产率足以确认稀土离子在掺钕激光介质中的均匀分散。对于使用沸石X的新制备的掺Nd的SiO2玻璃,量子产率在1.0 wt%时增加到50 +/- 3.4%,而普通生产的是7 +/- 0.5%。 (C)1997年Elsevier Science B.V.

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