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Nd:LuVO4晶体的生长及其性能研究 总被引:2,自引:0,他引:2
采用提拉(Czochralski)法生长了Nd:LuVO4晶体.利用液相反应法,以V2O5和NH4OH生成NH4VO3,Nd2O3、Lu2O3和HNO3生成Nd(NO3)3和Lu(NO3)3反应制备多晶料;所生长Nd0.01Lu0.99VO4晶体为16×20×21 mm3,质量超过40g.以X射线荧光分析仪测得其生长中各主要元素的分凝系数.其中Nd3+约为0.91,V3+和Lu3+接近1.还测定了其介电常数ε11=27.2,ε33=33.9(30℃,1kHz),以同步辐射X射线白光形貌术观察了其内部质量. 相似文献
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利用商群对称分析法分析了Nd:LuVO4晶体的晶格振动模分类,测量了Nd:LuVO4晶体的红外光谱和拉曼光谱,从测定的谱线中指认了该晶体的振动模,理论与实验符合良好.测量了Nd:LuVO4晶体的热膨胀系数,a向、b向和c向的热膨胀系数分别为 1.7×10-7/K 、1.5×10-7/K和9.1×10-7/K.测量了比热,其值约为0.48J/g·K.测量了热传导率,其值沿<100>方向为6.2W/m·K,沿<001>方向为7.9W/m·K.这些参数显示该晶体是一种热学性能优良的激光晶体. 相似文献
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采用助熔剂自发成核法生长了La: NdPO4晶体,采用X射线衍射技术表征了晶体的物相结构,采用红外和拉曼散射技术研究了晶体的品格振动特性,主要结论为:生长的晶体为单斜晶系,P21/n空间群;对实验观测到的振动模进行了指认,其中高频模主要为PO4四面体的内振动模.由于晶体结构缺陷和某些内、外振动模的耦合等原因,观测到的振动模数量少于理论预测值.通过比较La: NdPO4和NdPO4晶体的声子谱得出其晶格振动特性基本一致,但由于Nd比La的原子半径小,Nd和PO4之间的作用力增强,从而使PO4四面体"收缩",因此实验观测到La:NdPO4晶体的内振动模的波数较NdPO4晶体的蓝移. 相似文献
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Cr,Nd:GSAG是一种性能优良的激光晶体,但是关于它的LD泵浦激光性能的研究很少.用提拉法生长了Cr,Nd:GSAG晶体,测定了它的化学成分、结构,初步测试了它的激光性能.晶体的(111)面X射线摇摆曲线半高全宽为0.055°.采用Rietveld方法精修X射线粉末衍射谱得到了Cr,Nd:GSAG晶体的原子结构参数、温度因子等.Cr,Nd:GSAG的最强吸收峰位于808.6nm处,吸收截面为3.38×10-20cm2.808nm光激发下,Cr,Nd:GSAG的最强发射峰位于1060nm,发射截面为6.04×10-20cm2,并测得激光上能级4F3/2的荧光寿命为274μs.利用808nm连续波LD泵浦实现了1060nm的激光输出,在输入功率为8.88W时,最大输出功率为0.513W,斜效率为6.73;,光-光转换效率为5.78;.此外还讨论了Cr,Nd:GSAG晶体中的Cr3+与Nd3+之间的能量传递机理. 相似文献
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采用助熔剂自发成核法,以Li2CO3-2MoO3为助熔剂,生长出了Yb∶ NdPO4晶体.通过X射线粉末衍射和X射线能谱技术对所得的晶体进行了表征.结果表明,少量Yb3+掺入到了NdPO4晶体中,但并未改变NdPO4晶体的晶格结构.比较了Yb∶ NdPO4晶体和NdPO4晶体室温下的透过光谱.测量了室温下晶体的荧光光谱,泵浦光波长为332 nm.结果表明晶体的最强荧光发射峰位于995nm,归属于Yb3+从激发态2F5/2到基态2F7/2的电子跃迁.1059nm的发射峰归属于Nd3+从4 F3/2到4I11/2的电子跃迁.Nd3+的发射峰强度较弱,表明在室温下晶体中主要发生了Nd3+ →Yb3的能量传递. 相似文献
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双掺Nd,Ce∶YAG晶体相比传统的Nd∶YAG具有输出能量高、激光振荡阈值低的优点。近几年高能效固体激光器的发展对大尺寸、高质量Nd,Ce∶YAG晶体的需求越来越大。采用提拉法生长大尺寸Nd,Ce∶YAG时,极易出现包裹物和开裂缺陷。本文通过理论与实践相结合的方式分析了晶体在生长过程中产生缺陷的原因,并提出了解决办法,成功生长出直径ø50 mm等径长150 mm的高质量Nd,Ce∶YAG单晶。本研究可为批量化生长大尺寸Nd,Ce∶YAG晶体的质量改进提供方向和指导。 相似文献
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Czoehralski法成功生长了一系列不同Cd/Y的低掺杂Nd:YxGd1-xVO4混晶,并对它们的一些基本性质进行了比较,发现随着Gd含量的增加,晶体晶胞a,c轴常数呈线性增长,故YVO4和GdVO4晶体可以实现无限互溶。少量Gd掺杂可使混晶晶体比热和荧光寿命增大,并有效地增强了其荧光强度。我们对该晶体的低功率泵浦下的Cr^4 :YAG调Q激光性能也进行了研究,发现Nd:YxGd1-xVO4混晶具有良好调Q性能。 相似文献
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由于Nd3 离子半径0.112nm和Y3 离子半径0.101nm相差10.9%,使得Nd3 离子非常难于进入YAG晶体中。我们用温度梯度法生长了大尺寸高浓度(2.8 at%)的Nd:YAG晶体,同时与用提拉法Nd:GGG晶体进行了比较。分析了高浓度掺杂Nd:GGG和Nd:YAG晶体浓度猝灭问题。研究了不同浓度掺杂的猝灭效应。在同样的掺杂浓度下,我们发现它们的猝灭程度不同,其原因是两种晶体中ΔE(m is-)m和ΔE(m i s )m不同。 相似文献
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Bridgman growth of Nd:SGG (Sr3Ga2Ge4O14) crystals has been investigated for the first time. Pt crucible of ∅︁25mm×250mm with a seed well of ∅︁10mm×80 mm is used, and seed is SGG crystal of ∅︁10mm×50mm grown by Bridgman method in advance. The growth parameters are optimized as the furnace temperature is set to 1450∼1500°C, temperature gradient in the crystal‐melt interface is less than 25 K/cm and growth rate is less than 0.5mm/h. The Nd:SGG crystals with 25mm in diameter and 60mm in length are grown successfully from 1.5 to 8at% Nd3+ doped stoichiometric Sr3Ga2Ge4O14 melt. The distribution coefficient and concentration of Nd3+ in Nd:SGG crystals are obviously higher than those of Nd:YAG crystal. (© 2007 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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双掺离子在KTNNP晶体生长中的协同效应研究 总被引:3,自引:2,他引:1
本文采用高温溶液法生长了不同掺质浓度的较大尺寸掺Nd3+和Nb5+KTP(KTNNP)晶体,以X射线单晶衍射仪测定了所生长晶体的晶胞参数,以等离子发射光谱(ICP-AES)法系统测定了晶体中的掺质浓度。实验结果显示,掺Nd3+和Nb5+后,KTP晶体生长习性和形态发生了很大的变化,而且体系中Nd3+的分配系数明显增大,并随Nb5+浓度的增大而增大,从而体现了Nb5+对Nd3+的协同效应。另外,掺质后,晶体的单胞体积一般略有增大,但未呈现出规律性。 相似文献
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H. Saeedi M. Asadian Sh. Enayati N. Mirzaei I. Mashayekhi Asl J. Sabbaghzadeh 《Crystal Research and Technology》2011,46(12):1229-1234
In this paper, we report the growth of neodymium doped Gadolinium Gallium Garnet (Nd: GGG) crystal using Czochralski (CZ) method, and study the effects of crucible bottom deformation and thermal insulator thickness on the growth process and crystal quality. Garnet structure and <111> crystallography orientation of the crystal were confirmed by the X‐Ray diffraction (XRD) analysis. Macroscopic defects, residual stresses, quality, and homogeneity of the crystals were investigated by means of parallel plane polariscope and laser fizeau interferometer respectively and the results compared together. Experimental observations show that the crucible bottom deformation from flat to convex, and decreasing the thickness of zirconia insulator under the crucible result in the formation of lateral cores and increasing the crystal inhomogeneity and tensions, leading to the decrease of the crystal quality. (© 2011 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献
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V. Kannan R. Bairava Ganesh R. Sathyalakshmi N. P. Rajesh P. Ramasamy 《Crystal Research and Technology》2006,41(7):678-682
Single crystals of pure and Lanthanum added KDP crystals were grown from aqueous solution. The influence of La3+ ions in KDP crystals is studied. Isolated centers are formed by La3+ ions in KDP structure along (100) plane. La3+ ions incorporated into superficial crystal growth layer and slightly affect the growth process as they generate weak lattice stresses. The creation of these weak lattice stress is confirmed by Vickers's micro hardness test. The HRXRD analysis showed reduced structural defects in the La added KDP in the (100) plane than pure KDP. The incorporation of La in the crystal was confirmed by EDAX analysis. The Kurtz's powder SHG efficiency was found to be 1.5 times that of pure KDP. The UV‐Vis transmission spectra of La added KDP showed excellent transmittance from 1100 nm to 340 nm and did not show any change in lower cutoff wavelength with respect to pure KDP. Laser damage threshold value has been determined using Q‐switched Nd:YAG laser operating at 1064 nm and with 65 ns pulses in single shot mode. (© 2006 WILEY‐VCH Verlag GmbH & Co. KGaA, Weinheim) 相似文献