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1.
用一种新的测量方法在不同入射光强下同时观测了Fe∶LiNbO3 和 (Fe,Tb)∶LiNbO3 晶体中光致折射率变化Δns、吸收系数α和光电导σph与入射光强I的依赖关系 ,并从理论上对观测结果给予了初步解释  相似文献   

2.
在 L i Nb O3中掺进 Fe2 O3生长了 Fe∶ Li Nb O3晶体。对晶体进行氧化、还原处理 ,测试了 Fe∶ Li Nb O3晶体的吸收光谱以及 Li Nb O3和 Fe∶ L i Nb O3晶体的拉曼光谱 ,研究了氧化还原处理对晶体的光谱影响。  相似文献   

3.
Optics and Spectroscopy - We have observed that LiNbO3:Mg (0.19–5.91 mol % MgO) crystals experience rearrangements in their defect structure with increasing concentration of Mg and exhibit...  相似文献   

4.
Holographic storage properties of iron-doped and cerium/iron-doped LiNbO3 with different doping concentrations and treatment conditions have been measured for different recording wavelengths. The results show that at recording wavelengths of 532 nm and 633 nm the holographic storage properties of Ce:Fe:LiNbO3 are generally better than those of Fe:LiNbO3.  相似文献   

5.
掺锌LiNbO_3晶体的光谱性质   总被引:1,自引:0,他引:1  
在 Li Nb O3 中掺进 2 mol% ,4mol% ,6 mol% ,8mol%的 Zn O,生长 Zn(2 mol% ) :Li Nb O3 ,Zn(4mol% ) :Li Nb O3 ,Zn(6 mol% ) :Li Nb O3 和 Zn(8mol% ) :Li Nb O3 晶体 ,测试 Li Nb O3 和掺锌Li Nb O3 晶体的透射光谱。Li Nb O3 和掺锌 Li Nb O3 晶体在 35 0— 90 0 nm的范围内都是透明的。Zn:Li Nb O3 晶体的吸收边发生紫移。对 Zn:Li Nb O3 晶体吸收边紫移的机理进行探讨。  相似文献   

6.
用紫外可见光谱(UV/Visible Spectra)测试并研究了坩埚下降法生长的LiNbO3、Fe:LiNbO3,以及Zn:Fe:LiNbO3晶体的吸收特性。分析了产生这些吸收特性的原因以及与工艺生长方法的内在联系。研究结果表明:LiNbO3单晶沿晶体生长方向,其紫外吸收边向长波方向移动,且在350—450nm波段的吸收也逐渐增大,这是由于Li的分凝与挥发,逐渐产生缺锂所造成的;在Fe:LiNbO3单晶中观察到Fe^2 离子在480nm附近的特征吸收峰,并发现沿生长方向,Fe^2 离子的浓度逐渐增加,这与提拉法生长得到的晶体不同;在Fe:LiNbO3单晶中掺入质量分数为1.7%ZnO后,吸收边位置发生蓝移,而掺杂质量分数达到3.4%时,观察到有红移现象。Fe^2 离子在Zn:Fe:LiNbO3单晶中的浓度与ZnO掺杂量有密切关系。在掺杂质量分数1.7%ZnO的Fe:LiNbO3单晶中,Fe^2 离子从底部到顶部的浓度变化比在掺杂质量分数3.4%ZnO晶体中大,这是由于Zn^2 抑制Fe^2 离子进入Li位的能力随掺杂量的增加而逐渐减弱造成的。就该下降法工艺技术对Fe^2 离子在晶体中的浓度分布的影响作了分析。  相似文献   

7.
LiNbO3:Ru晶体的光折变特性研究   总被引:1,自引:1,他引:1  
采用丘克拉斯基法生长了单掺杂的LiNbO3∶Ru晶体,并对其作氧化处理。实验研究了LiNbO3∶Ru晶体二波混频条件下光栅记录特性和波长的依赖关系;并且研究了氧化处理对其透射谱和光栅记录特性的影响。研究结果表明,LiNbO3∶Ru晶体的最佳记录波长为458 nm;氧化处理会增加LiNbO3∶Ru晶体对光的吸收,同时提高光栅记录的灵敏度和饱和衍射效率,表现了不同于LiNbO3∶Fe晶体的氧化态依赖特性。分析认为,LiNbO3∶Ru晶体的反常氧化态依赖特性可能是由于出现了电子通道效应的暗衰减机制,以及Ru存在多个价态所造成的。  相似文献   

8.
Zn:Fe:LiNbO3晶体全息存储性能研究   总被引:7,自引:7,他引:0  
以提拉法生长Zn(1mol%):Fe:LiNbO3, Zn(4mol%):Fe:LiNbO3,Zn(7mol%):Fe:LiNbO3晶体.Zn:Fe:LiNbO3晶体随着Zn2+浓度的增加,抗光致散射能力增加,Zn(7mol%):Fe:LiNbO3晶体抗光致散射能力比Fe:LiNbO3晶体提高两个数量级以上.测试了Zn:Fe:LiNbO3晶体衍射效率、响应时间.以Zn(7mol%):Fe:LiNbO3晶体作为存储元件,Zn(4mol%):Fe:LiNbO3晶体作为位相共轭镜,进行全息关联存储试验.试验结果显示出成像质量好、图像清晰完整、噪音小等优点.研究了Zn:Fe:LiNbO3晶体全息存储性能增强的机理.Zn(4mol%):Fe:LiNbO3晶体具有全息存储性能最佳的综合指标.  相似文献   

9.
郑威  周玉祥  刘彩霞 《光子学报》2003,32(12):1492-1494
在LiNbO3中掺进CeO2和Co3O4,以Czchralski技术首次生长Ce:Co:LiNO3, Ce:LiNbO3, Co:LiNbO3晶体.通过测试Ce:LiNbO3, Co:LiNbO3和Ce:Co:LiNbO3晶体的指数增益系数, 位相共轭反射率和响应时间,计算晶体的有效载流子浓度和光电导.Ce离子能提高LiNbO3晶体光折变灵敏度,Co离子能提高LiNbO3晶体的响应速度和抗光致散射能力,从而Ce:Co:LiNbO3晶体具有较高的指数增益系数,位相共轭反射率,响应速度.Ce:Co:LiNbO3晶体具有优良的光折变性能.  相似文献   

10.
在 LiNbO3中掺进In2O3和Nd2O3, 以Czochralski技术生长了In∶Nd∶LiNO3晶体. 通过光斑畸变法测得In∶Nd∶LiNbO3晶体的光损伤阈值为1.98×104 W/cm2, 比Nd∶LiNbO3晶体的1.6×102 W/cm2高两个数量级以上;晶体吸收光谱的测试表明, In∶Nd∶LiNbO3晶体的吸收边相对Nd∶LiNbO3晶体发生紫移. 研究了In∶Nd∶LiNbO3晶体的倍频性能, 结果表明, In∶Nd∶LiNbO3晶体的相位匹配温度在室温附近, 倍频转换效率比Nd∶LiNbO3晶体提高二倍.  相似文献   

11.
Angle-multiplexed hologram storage in LiNbO(3):Tb, Fe   总被引:3,自引:0,他引:3  
We have performed hologram multiplexing with a cw laser at lambda=532 nm in a near-stoichiometric LiNbO(3) :Tb, Fe crystal that exhibits a visible absorption band induced by UV light. When 50 plane-wave holograms were angle multiplexed from the UV preexposed state, the recording sensitivity gradually decreased, owing to bleaching of the induced absorption. However, a conventional recording schedule of multiplexing many holograms of equal diffraction efficiency can be used in this photochromic material. The gradual decrease in recording sensitivity throughout multiplexing can be compensated for by the increased erasure-time constants of later-written holograms. An M/# of 1.73 was obtained in a crystal of 3.3-mm thickness.  相似文献   

12.
掺Ce,Fe系列LiNbO3晶体光折变效应光存储特性   总被引:5,自引:4,他引:5  
研究了系列Ce:Fe掺杂以及不同后处理态(生长态、还原态和氧化态)铌酸锂晶体的透过率光谱和光折变全息存储特性。实验结果表明单掺Ce铌酸锂晶体具有较好的图像存储质量和较宽的透过率光谱范围,二波耦合增益相对较低;高掺杂铌酸锂样品的透过率光谱范围较窄,光折变二波耦合增益较低。晶体的后处理对铌酸锂样品的光折变特性影响明显,双掺Ce:Fe还原态铌酸锂晶体具有较高的二波耦合增益;氧化态样品具有较大的透过率光谱范围;还原态样品具有较大的光折变二波耦合增益特性。实验结果还表明在同种样品中难于同时获得大的二波耦合增益和图像存储质量。  相似文献   

13.
A spontaneous decrease of photorefraction (quasi-breakdown) has been studied in LiNbO3−Fe (0.1 wt%) crystals. It is shown that the quasi-breakdown effect depends on the crystal environment (air, argon) and is absent in a liquid dielectric medium. Quasibreakdown can be avoided reducing the diameter of the light beam from a He−Ne laser. The critical value of birefringence change for quasi-breakdown decreases with growing temperature. The quasi-breakdown effect is also observable after illumination, in the dark. It is shown that quasi-breakdown can be explained by the recombination of light-induced space charge carriers at the surface or in the environment (air, argon) near the crystal surface. The erasure of photorefraction with quasi-breakdown is performed under under uniform illumination of the crystal with visible light.  相似文献   

14.
双掺杂LiNbO3晶体中的稳态空间电荷场   总被引:4,自引:2,他引:2  
建立了包括扩散、漂移和光伏打三种输运机制下双掺杂LiNbO3晶体在用双色光进行光存储的带输运方程,并得出了小调制度下稳态空间电荷场的分析解。对双色光的光强比、体光栅的波矢、双掺杂的浓度和晶体的 氧化还原程度对空间电荷场的影响进行了数值计算和讨论。  相似文献   

15.
Experimental studies of IRS by polaritons in LiNbO3 are reported for the first time. In compliance with the classification of IRS-scattering geometries by polaritons in uniaxial crystals [3] for different polarisation directions of laser and anti-Stokes continuum two A1-type polaritons and also E-type-polaritons of the upper and the lower ordinary dispersion branches, respectively, could coherently be generated. Introducing a new polariton specific excitation state instead of the mechanic vibration the shortened IRS equations without small signal approximation are solved in the stationary case and for “responseless” polariton fields. The increase of the laser field and the decrease of the anti-Stokes field show for αpx ? 1 the same behaviour as Stokes growth and laser depletion, respectively, in the case of SRS by dipole inactive levels. Model calculations show the necessity of the used intra cavity arrangement for photographic registration of IRS-polariton spectra.  相似文献   

16.
Raman spectra of LiNbO3: MgO crystals have been obtained and compared with Raman spectra of pure LiNbO3 crystals. For both of the two kinds of Raman active modes (4A1+9E), no changes of the numbers, frequency-shifts, and relative intensities of the Raman spectral lines are found. However, it is observed that some modes coupled to each other at room temperature. The observed modes coupling phenomena, disappeared at low temperature. It is shown from these results that the Raman spectral lines of A1 (TO) and E (TO) vibrational modes are mainly determined by the (NbO6) oxygen octahedra characteristic groups of LiNbO3 crystals.  相似文献   

17.
研究了LiNbO3∶Cr∶Cu晶体的吸收特性,发现LiNbO3∶Cr∶Cu(含0.14 wt.% Cr2O3 和 0.011 wt.% CuO)晶体存在两个明显的吸收峰,中心波长分别位于480 nm和660 nm; 随着Cr的含量逐渐减小,Cu的含量逐渐增大,短波段不存在明显吸收峰,掺Cr的含量越大,中心波长在660 nm处的吸收越大;633 nm红光虽然位于中心波长为660 nm的吸收峰内,但它无助于光折变过程.分别采用390 nm紫外光和488 nm蓝光作为敏化光,514 nm绿光作为记录光的记录方案,实现了非挥发全息记录,掺入适量的Cr( 比如NCr=2.795×1025 m-3,NCr/ NCu=1)有助于全息记录性能的提高.  相似文献   

18.
在LiNbO3中掺进0.015mass%MnCO3和 0.1mass%CeO2,以Czchralski法生长Li/Nb比为1.38的近化学计量比Ce∶Mn∶LiNbO3(Ce∶Mn∶SLN)晶体和Li/Nb比为0.946的同成分Ce∶Mn∶LiNbO3(Ce∶Mn∶CLN)晶体.测试了晶体的红外光谱和紫外可见吸收光谱,讨论了Ce∶Mn∶SLN晶体OH-吸收峰和吸收边移动机理.利用二波耦合光路测试了晶体的指数增益系数,Ce∶Mn∶SLN晶体指数增益系数Γ达到27 cm2-.同时,研究了Ce∶Mn∶SLN指数增益系数提高的机理.  相似文献   

19.
20.
报道了在铌酸锂晶体中实现紫外激光诱导畴反转的实验。在一定外加均匀电场下,铌酸锂晶体中通过波长365nm的紫外激光,由于紫外光的照射降低了矫顽电场只在通光区实现畴反转。研究表明,该方案可用于周期性极化铌酸锂的制备,并有望成为制作精细周期性畴结构的有效技术方案。  相似文献   

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