共查询到20条相似文献,搜索用时 23 毫秒
1.
We detect the photo-induced carriers in near-stoichiometric iron doped LiNbO3 crystal by the holographic technique. The results show that the dominant carriers are electrons in the sample with Li/Nb ratio of 0.9988. By analysis of the OH^- absorption spectra of the crystal, we contribute the electron domination in near-stoichiometric Fe-doped LiNbO3 crystal to the existence of NbLi which provides the anti-site defect to Fe^2+. 相似文献
2.
The phenomena of acoustic emission in LiNbO3:Fe:Ce crystals have been observed in the process of light-induced quasi-breakdown. It is found that the ultra-high frequency acoustic signal introduced into the crystal is modulated by the low frequency acoustic waves. Its frequency increases with the increase of the intensity of incident light and its jump period of breakdown is the same as that of the photovoltaic current Ic, the change of light-induced refractive index △n and the diffracted light intensity L. This phenomenon has been analysed in this paper, which is caused by the inverse piezoelectric strain effect of the jump of space charge field during the quasi-breakdown. 相似文献
3.
Fe:LiNbO3和(Fe,Tb):LiNbO3晶体中入射光强对光折变性质的影响 总被引:2,自引:0,他引:2
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△ns、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
4.
6.
7.
Microstructure on Surface of LiNbO3:Fe Induced by a Single Ultra—Short Laser Pulse 总被引:2,自引:0,他引:2 下载免费PDF全文
A tightly focused femtosecond Ti:sapphire laser pulse is used to initiate micro-explosions on the surface and internal to an Fe:LiNb03 crystal. The resulting structure is morphologically different from that induced in an isotropic sample such as fused silica. The regular pyramid and irregular pyramid craters on the surface of the sample are produced at different positions of focal points. The craters suggest vaporization of materials in the process of micro-explosion due to the expansion of high temperature plasma. The embossment pyramids on the surface present the dynamical process of large volume material displacements under high temperature and pressure, and recrystallization of anisotropy crystal materials. 相似文献
8.
We perform a comprehensive experimental study on holographic and thermal-fixing characteristics of Zn:Fe:LiNbO3 The measured hologram decay time constants, respectively caused by optical readout and under dark condition, with thermal fixing are 15 times and 75 times longer than that obtained without thermal fixing. This suggests that Zn:Fe:LiNbO3 crystals are suitable for thermal fixing. Multiplexed recordings of 300 holograms using different thermal fixing schemes verify that a proper multiplexing scheme such as track-division thermal-fixing scheme for disc-type holographic storage can effectively compensate for the negative effect of zinc-doping on the dynamic range, thus the storage density is enhanced. 相似文献
9.
在Fe∶LiNbO3中掺进MgO和Fe2 O3以提拉技术生长Mg∶Fe∶LiNbO3晶体 对晶体进行极化和还原处理 测试晶体的吸收光谱 ,Mg∶Fe∶LiNbO3晶体吸收边相对Fe∶LiNbO3晶体发生紫移 测试晶体的红外光谱 ,Mg∶(5mol % )Fe∶LiNbO3晶体OH 吸收峰由Fe∶LiNbO3晶体的 3482cm- 1移到35 34cm- 1 采用锂空位模型阐述Mg∶Fe∶LiNbO3晶体 ,吸收边和OH- 吸收峰移动的机理 测试晶体的抗光致散射能力 Mg∶(5mol% )Fe∶LiNbO3晶体抗光致散射能力比Fe∶LiNbO3晶体提高一个数量级以上 测试晶体的衍射效率和响应时间 Mg∶Fe∶LiNbO3晶体响应速度比Fe∶LiNbO3晶体提高四倍 相似文献
10.
在Fe:LiNbO3中掺进MgO和Fe2O3以提拉技术生长Mg:Fe:LiNbO3晶体.对晶体进行极化和还原处理.测试晶体的吸收光谱,Mg:Fe:LiNbO3晶体吸收边相对Fe:LiNbO3晶体发生紫移.测试晶体的红外光谱,Mg:(5 mol%)Fe:LiNbO3晶体OH-吸收峰由Fe:LiNbO3晶体的3482 cm-1移到3534 cm-1.采用锂空位模型阐述Mg:Fe:LiNbO3晶体,吸收边和OH-吸收峰移动的机理.测试晶体的抗光致散射能力.Mg:(5 mol%)Fe:LiNbO3晶体抗光致散射能力比Fe:LiNbO3晶体提高一个数量级以上.测试晶体的衍射效率和响应时间.Mg:Fe:LiNbO3晶体响应速度比Fe:LiNbO3晶体提高四倍. 相似文献
11.
Dynamic Phase-Mapping of Domain Nucleation in MgO:LiNbO3 Crystal by Digital Holographic Interferometry 下载免费PDF全文
The quantitative phase-mapping of the domain nucleation in MgO:LiNbO3 crystals is presented by using the digital holographic interferometry. An unexpected peak phase at the beginning of the domain nucleation is observed and it is lowered as the spreading of the domain nucleus. The existence of the nucleus changes the moving speed of the domain wall by pinning it for 3 s. Such in-situ quantitative analysis of the domain nucleation process is a key to optimizing domain structure fabrication. 相似文献
12.
采用调Q Nd:YAG激光倍频光(0.532μm)泵浦温度调谐MgO:LiNbO_3晶体单、双谐振光参量振荡器(OPO包括DRO、SRO)的实验结果.双谐振(DRO)调谐范围达844.1~1411.3nm,最低泵浦阈值0.22mJ/pulse;单谐振(SRO)调谐范围达738.9~1032.2nm,最低泵浦阈值0.66mJ/pulse.最大能量转换效率为10.4%. 相似文献
13.
Improvement in refractive-index change in LiNbO3:Ce:Cu by applying an external electric field 下载免费PDF全文
By jointly solving two-centre material equations with a nonzero external electric field and coupled-wave equations, we have numerically studied the dependence of the non-volatile holographic recording in LiNbO3:Ce:Cu crystals on the external electric field. The dominative photovoltaic effect of the non-volatile holographic recording in doubly doped LiNbO3 crystals is directly verified. And an external electric field that is applied in the positive direction along the c-axis (or a large one in the negative direction of the c-axis) in the recording phase and another one that is applied in the negative direction of the c-axis in the fixing phase are both proved to benefit strong photorefractive performances. Experimental verifications are given with a small electric field applied externally. 相似文献
14.
15.
16.
17.
光色效应(Fe,Mn):LiNbO3晶体非挥发性全息存储自衍射效应的实验研究 总被引:2,自引:0,他引:2
在双掺杂(Fe,Mn):LiNbO3晶体光色效应非挥发性全息存储实验中,观测到光束耦合作用导致的自增强和自衰减效应,根据这种自衍射效应,归纳了四种记录和光固定实验组合方案,实验结果表明,在记录和光固定过程中利用自增强效应得到的最高衍射效率为利用自衰减效应得到的衍射效率的两倍左右,说明在实际应用中必须考虑和利用自增强效应。 相似文献
18.
在确定Cu在LiNbO3晶体中对应于365nm和633nm的激发系数、复合系数、光伏系数的基础上,采用龙格-库塔(Runge-Kutta)数值方法理论研究了双掺杂(Fe,Cu):LiNbO3晶体的深浅能级的掺杂组分比、氧化-还原状态对双色全息存储的记录灵敏度和动态范围的影响,并探讨了同时取得尽可能大的灵敏度和动态范围的晶体条件。结果表明,为了同时得到较大的记录灵敏度和动态范围,在实际应用中选用浅能级掺杂浓度为5.0×10^25m^-3,深能级掺杂浓度为3×10^24~3×10^25m^-3之间的弱氧化晶体是合适的。 相似文献
19.
采用电光调Q脉冲Nd:YAG激光的二次谐波(532nm)抽运温度调谐的MgO:LiNbO3晶体光学参量振荡器,调谐范围达800nm-1750nm.在单谐振运转条件下,抽运阈值为21.5mJ/pulse,最大抽运能量为58mJ时输出为6.45mJ,在大信号情况下的能量转换效率达11%,输出线宽1nm左右。 相似文献
20.
分别采用514 nm绿光、488 nm蓝光和390 nm紫外光作为敏化光,633 nm红光作为记录光,详细研究了敏化光波长对氧化(Fe,Ni):LiNbO3晶体全息记录性能的影响.结果表明:随着敏化光波长的逐渐减小,氧化(Fe,Ni):LiNbO3晶体的非挥发全息记录性能逐渐优化,390 nm紫外光是这三种敏化光中最优的敏化光.考虑敏化光的吸收,为了在双中心全息记录中获得最优的性能,应当选择合适波长的敏化光:一方面短波长敏化光能有效地敏化深中心;另一方面短波长敏化光的吸收太强(如对光折变效应无用的基质吸收),不能沿厚度方向有效地敏化晶体,所以实际上需折衷考虑,并从理论上给予了解释. 相似文献