556 resultados para annealing Al2O3
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利用气相传输平衡技术(VTE)和后退火处理工艺在(0001)蓝宝石衬底上获得了高度[100]取向的γ-LiAlO2薄膜.X射线衍射表明是由单相的γ-LiAlO2所组成,此薄膜经850~900℃/120h空气中退火处理后显示出高度的[100]取向,这一实验结果意味着有望通过VTE方法制备用于GaN基器件外延生长的γ-LiAlO2(100)-Al2O3(0001)复合衬底.
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Visible upconversion luminescence was observed in Cr3+: Al2O3 crystal under focused femtosecond laser irradiation. The luminescence spectra show that the upconversion luminescence originates from the E-2-(4)A(2) transition of Cr3+. The dependence of the fluorescence intensity of Cr3+ on the pump power reveals that a two-photon absorption process dominates in the conversion of infrared radiation to the visible emission. It is suggested that the simultaneous absorption of two infrared photons produces the population of upper excited states, which leads to the characteristic visible emission from E-2 state of Cr3+.
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The broadband emission in the 1.2 similar to 1.6 mu m region from Li2O-Al2O3-ZnO-SiO2 ( LAZS) glass codoped with 0.01mol.% Cr2O3 and 1.0mol.% Bi2O3 when pumped by the 808nm laser at room temperature is not initiated from Cr4+ ions, but from bismuth, which is remarkably different from the results reported by Batchelor et al. The broad similar to 1300nm emission from Bi2O3-containing LAZS glasses possesses a FWHM ( Full Width at Half Maximum) more than 250nm and a fluorescent lifetime longer than 500 mu s when excited by the 808nm laser. These glasses might have the potential applications in the broadly tunable lasers and the broadband fiber amplifiers. (c) 2005 Optical Society of America.
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ZnO films were grown on (0 0 0 1) LiNbO3 substrates by metal organic chemical vapor deposition (MOCVD). Annealing of ZnO films was performed in air for I h at 800 degrees C. The effects of annealing on the structural and optical properties of ZnO thin films on LiNbO3 substrates were investigated using X-ray diffraction (XRD), atomic force microscopy (AFM) and photoluminescence (PL) measurements. XRD patterns and AFM showed that the as-grown and the annealed ZnO films grown on LiNbO3 substrates had c-axis preferential orientation, the crystallinity of the ZnO films grown on LiNbO3 Substrates was improved, and the grain size increased by annealing. The PL spectra showed that the intensity of the UV near-band-edge peak was increased after annealing, while the intensity of visible peak (deep-level emission) decreased. (c) 2005 Elsevier B.V. All rights reserved.
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对透光性良好的Cr^3+:Al2O3透明多晶陶瓷的光谱性能进行了研究,其吸收光谱中吸收峰与单晶红宝石相一致,按吸收光谱和Tanabe-Sugano能级图,算出其晶场强度参数Dq及Racah参数B分别为1792cm^-1,689cm^-1,Dq/B=2.6,陶瓷中Cr^3+离子所处格位的晶体场强比单晶弱一些,但Cr^3+:Al2O3透明陶瓷仍属于强场晶体材料;当Cr^3+掺杂浓度到达0.8wt%时,陶瓷的发射谱仍保持较好的R线发射;随Cr^3+掺杂浓度的增大,激发峰位发生“红移”.在Cr^3+:Al2O3透
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The effects of gamma irradiation on as-grown 5 at% Yb:YAlO3 (YAP) and air annealing on gamma-irradiated 5 at% Yb: YAP have been studied by the difference in the absorption spectra before and after treatment. The gamma irradiation and air annealing led to opposite changes of the absorption properties of the Yb: YAP crystal. After air annealing, the gamma-irradiation effects were totally removed over the wavelength range 390-800 nm and the concentrations of Fe3+ and Yb3+ were slightly increased. For the first time, the gamma-irradiation-induced valence changes between Yb3+ and Yb2+ ions in Yb: YAP crystals have been observed. (c) 2005 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim.
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Five absorption hands, at 227, 300 340, 370 and 457nm, were observed in the optical absorption spectrum of Ce:Y3Al5O12 (Ce:YAG) crystals grown by the temperature gradient technique (TGT). The absorption bands at 227, 340, and 457 nm were identified Lis belonging to the Ce3+ -ion in the YAG crystal. A near UV optical emission band at 398nm was observed. with an excitation spectrum containing two bands, at 235 and 370nm. No fluorescence was detected under 300 nm excitation. The pair of absorption bands at 235 and 370 nm and the absorption band at 300 nm were attributed to the F- and F+-type color centers, respectively. The color centers model was also applied to explain the spectral changes in the Ce:YAG (TGT) crystal, including the reduction in the Ce 31 -ion absorption intensity, after annealing in an oxidizing atmosphere (air). (C) 2004 Elsevier B.V. All rights reserved.
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Transparent polycrystalline MgO and TiO2 codoped Al2O3 ceramics were fabricated by conventional solid-state pressureless processing. The absorption, emission and excitation spectra of ( Mg, Ti : Al2O3 ceramics were measured. Owing to charge compensation of Mg2+, only UV absorption around 250nm was observed due to O2- -> Ti4+ charge transfer transitions (CT) when Ti content was low. As a result, the emission peaks of isolated Ti4+ ion located at 280-290nm and 410-420nm were observed. Besides absorption peak of V, ion, the characteristic absorption peak of V, ion centered at 490nm was observed in Mg, Ti) : Al2O3 ceramics when Ti content was high. The emission spectra of Ti3+, ion in polycrystalline Al2O3 ceramics coincide with that of Ti: Al2O3 single crystal.
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Cr-doped and Mg, Cr-codoped Al2O3 crystals were grown by Czochralski method. The latter has a broad absorption peak in 900-1600nm region. We investigated the change of the absorption band with annealing under different atmospheres or temperatures. Through establishing a structure defect model, we successfully interpreted all the experiment results and confirmed that the extremely broad infrared absorption band belonged to Cr4+, which should occupy the octahedral sites in Al2O3.
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The absorption spectra of the undoped Y2SiO5 and Eu3+-doped Y2SiO5 crystals grown by the Czochralski technique were compared before and after annealing and, similarly, the unannealed and annealed crystals after gamma-ray irradiation. The absorption bands of Eu2+ ions with peaks at 300 and 390 nm were observed in the as-grown Y2SiO5:Eu3+ crystal. These peaks were more intense in H-2-annealed and irradiated Y2SiO5:Eu3+ crystals. The additional absorption peaks at 260 and 320-330 nm which were attributed to F color centers and O- hole centers were observed in irradiated undoped Y2SiO5 and Y2SiO5:Eu3+ crystals, respectively. (c) 2005 Elsevier B.V. All rights reserved.
Resumo:
用脉冲激光沉积法(PLD)在MgO(100)、a-Al2O3(0001)和MgAl2O4(111)衬底上沉积了ZnO薄膜,测量了它们的发射光谱,观察到430nm的蓝光发射,并研究了退火、衬底和激发波长对ZnO薄膜这一蓝光发射的影响。指出ZnO薄膜中430nm的蓝光发射是由锌填隙原子缺陷能级到价带顶能级间的跃迁以及电子从氧空位浅施主能级到价带顶能级间的跃迁两种机理共同作用的结果。在MgO衬底上沉积的ZnO薄膜在350nm光激发下蓝光发射峰最强。
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本文研究了不同掺Ti^3+浓度对温梯法生长的Ti:Al2O3晶体吸收光谱、荧光光谱和X射线衍射光谱的影响。根据吸收光谱提出了一个色心模型。对比了样品各处420nm荧光谱,发现掺Ti^3+浓度越大,该处荧光强度越弱,同时解释了420肿处荧光峰的起源。对比了样品各处720nm处的荧光谱,发现掺Ti^3+浓度越大,该处荧光强度越强。X射线衍射谱(XRD)表明,衍射峰强度随掺Ti^3+浓度的增大而逐渐增强。
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采用传统无压烧结工艺制备出透明性良好的掺Ti氧化铝陶瓷;测定了该陶瓷的吸收光谱、荧光光谱和激发光谱。结果表明,掺Ti氧化铝透明陶瓷样品在Mg与Ti掺入离子的摩尔比(NMg/NTi)较小时,表现出Ti^3+离子的490nm特征吸收峰,即^2T2→^2E跃迁产生的宽带吸收;NMg/NTi较大时,陶瓷样品吸收光谱中不存在Ti^3+离子吸收,其250nm处吸收为O^2-→Ti^4+的转移吸收。掺Ti氧化铝透明陶瓷样品Ti^3+离子的发射谱线与单晶的相吻合,同时Ti^3+在氧化铝陶瓷中分布很均匀,且Ti^3+浓度较
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用脉冲激光沉积法在Al2O3(0001)衬底上沉积了ZnO薄膜。衬底温度分别为300℃、400℃、500℃、600℃和700℃。利用X射线衍射(XRD)和光致发光谱(PL)对薄膜的结构和光学性能进行研究。X射线衍射的结果表明在不同温度下生长的ZnO薄膜均具有高度c轴择优取向,衬底温度400℃时,膜的应力较小质量较高。ZnO薄膜有很强的紫外发光峰,紫外发光峰的强度与衬底温度密切相关,并发现当衬底温度从300℃增到400℃时,紫外发射峰出现6nm的蓝移。
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采用传统无压烧结工艺制备出透明性良好的掺Cr的Al2O3透明陶瓷;测定了其吸收光谱和荧光光谱,发现在Al2O3六配位的八面体结构中,除了有Cr^3+离子的特征吸收峰外,由于有Mg^2+的电荷补偿作用,也有Cr^4+离子,Cr^4+的荧光发射峰位于1223nm附近,与Cr^4+在四面体中的发光行为一致。但其荧光发射峰较窄,半高宽△λ仅为37nm。