共查询到19条相似文献,搜索用时 125 毫秒
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采用外加电场法制备了LiNbO3单晶周期畴结构. 在对不同尺寸周期畴的反转电流进行比较研究的基础上,提出了一种确定反转畴成核时间和纵向贯穿速率的方法. 根据这一方法,得到在电场强度为25.1kV/mm,脉冲宽度为50 ms的脉冲方波作用下,LiNbO3单晶反转畴的成核时间约为80ns,纵向贯穿速率约为0.1667m/s.
关键词:
3单晶周期极化')" href="#">LiNbO3单晶周期极化
反转电流
反转畴成核时间
反转畴纵向贯穿速率 相似文献
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我们通过测定MgO在同成分LiNbO3中的有效分凝系数、相位匹配温度与MgO浓度之间的关系,找到了使Mg:LiNbO3晶体的相位匹配温度达到最高的掺MgO配方,并克服了Mg:LiNbO3晶体在高掺杂生长时易出现生长条纹和脱溶等问题,从而生长出了抗光折变能力强,光学均匀性良好的Mg:LiNbO3晶体。用于连续泵浦Nd:YAG声-光调Q腔内倍频时,获得了平均功率最高达2瓦的二次谐波输出。
关键词: 相似文献
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利用外加电场极化的方法,分别研究了三种不同方式布置的极化电极对C向切割LiNbO3< /sub>晶体极化反转畴扩张的影响.实验结果表明在相同极化条件下,当极化电极长度方向与六边 形反转畴一对边呈90°和0°角时,极化扩张速度分别为0.089μm/ms和0.011μm/ms.实验结果揭示,为了有效地控制极化占空比,在制备一维准相位匹配LiNbO3晶体时应 避免极化电极与六边形反转畴壁中一对边呈90°的情况.
关键词:
周期极化
极化扩张
准相位匹配 相似文献
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铁电单晶体自发极化引起的强周期性表面电场可能用来代替Wiggler磁铁产生自由电子激光。但落在铁电晶体表面上的自由电子将逐渐把表面势屏蔽掉。本文提出一个抗屏蔽措施:在LiNbO3极化晶面上每一个正极化畴区铺上一层绝缘膜,在上面再覆盖一层接地导体膜,可以防止电子对极化晶面的屏蔽。本文证明了在导体膜每部分两表面应电荷之和为零,落在上面的自由电子将立刻逃逸入地。
关键词: 相似文献
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用气相输运平衡技术成功地制备出了近化学计量组分的Er∶LiNbO3晶体,系统 地研究了该 晶体的吸收边移动、可见—红外透射谱、荧光光谱的物理特性.与同成分Er∶LiNbO3 sub>晶体 相比, 近化学计量组分Er∶LiNbO3晶体的吸收边出现了“蓝移”;OH- sup>吸收带明显减弱 ;在可见—近红外波段呈现出更高的透过率;同时Er3+离子的发光强度也明显 提高. 这些结果表明近化学组分的Er∶LiNbO关键词:
近化学组分掺铒铌酸锂晶体
- 吸收带')" href="#">OH-吸收带
透射谱
荧光光谱 相似文献
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本文报道了一组不同Li/Nb比和另一组不同掺Mg浓度的LiNbO3晶体室温OH-吸收带的实验结果,观察到OH-吸收带的三峰结构及其随Li/Nb比的变化,以及重掺Mg晶体中(6mol%MgO)OH-吸收带转变为双峰结构,并向高能端移动54cm-1。根据LiNbO3的晶体结构以及Abrahams和Smyth的缺陷结构模型,对化学计量晶体、一致熔化晶体和掺Mg晶体分别进行讨论。并提出重掺Mg晶体中OH-吸收带向高能端的移动可能是由于当掺Mg浓度超过阈值后Mg2+离子开始进入Nb位而引起的。
关键词: 相似文献
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D. Zhang X. Chen Y. Jin X. Cao D. Zhu Y. Wang G. Ding Y. Cui C. Chen Z. Wu G. Lan 《Applied Physics A: Materials Science & Processing》2001,72(1):95-102
Raman spectra of Er:LiNbO3 crystal and Ti-diffusedEr:LiNbO3 strip waveguide, in which the Li/Nb ratio was altered using a vapor-phase equilibration (VPE) technique, were measured at
room temperature in the wave-number range 50–3500 cm-1. Both 488 and 514.5 nm radiations were used to excite Raman scattering, A1(TO) and E(TO) modes were recorded at backward scattering geometry. The results indicated that the lattice vibrational spectra
of the as-grown Er:LiNbO3 are almost the same as those of pure LiNbO3 except for the little shift of the peak position and the change of relative intensity of some peaks. In comparison with the
spectra of as-grown Er:LiNbO3 crystal the vapor-phase equilibrated Er:LiNbO3 and Er:Ti:LiNbO3 crystals in the lattice vibrational region exhibit the following features: firstly, Raman peaks become narrow, indicating
that the VPE process has brought Er:LiNbO3 and Er:Ti:LiNbO3 crystals closer to a stoichiometric composition; secondly, relative intensity of some peaks varies with the VPE time; and
finally, slight blue shifting in peak position was observed. Some of these features were correlated with the NbO6 octahedra and with the site distribution of the doped Er ions. In addition, green fluorescence peaks and/or bands associated
with the electron transitions 2
H
11/2?4
I
15/2 and 4
S
3/2?4
I
15/2 of the doped Er3+ were also observed. For 488 nm excitation they appear in the wavenumber range of 1200–3000 cm-1 and are well separated from lattice vibrational region; for 514.5 nm excitation, however, these fluorescence peaks shift
towards the low wavenumber region and overlap partially with the lattice vibrational spectra.
Received: 24 May 2000 / Accepted: 29 May 2000 / Published online: 13 September 2000 相似文献
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The specific heat of a NaNO2 sample has been measured between 2 K and 40 K in both single-domain and polydomain states. In this region the specific heat of the single domain sample follows exactly the T3 dependence. A clear excess contribution which in this temperature range has a temperature dependence between T and T2 has been detected for the polydomain sample. It is attributed to domain walls. 相似文献
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《光谱学快报》2013,46(4):437-442
The Raman Spectra of LiNbO3:MgO (6.7 mol%) at both low temperature and room temperature were studied. The results showed that the crystal structure has changed little after doping Mg+ +. At room temperature the lattice distorted a little, which caused the appearance of coupling phenomenon of some individual scattering peaks. As the temperature decreased, the coupling reduced gradually. 相似文献
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在忽略电子-声子相互作用的基础上,本文探讨了从能带波函数出发计算AB型晶体倍频系数的可能性。采用计算AB型晶体能带的近似方法——等价轨道法。计算了k=0点的倍频系数,然后通过带宽的修正,使k=0点的倍频系数近似地表为不同k点倍频系数的平均,这一平均值乘以第一布里渊区内k点的总数就是晶体的宏观倍频系数。计算了十七种闪锌矿型和纤维锌矿型晶体的倍频系数,计算值和实验值的吻合相当满意。从中得出几点有用的结论:(1)倍频系数的双能级跃迁模型对闪锌矿型结构是适用的;但对纤维锌矿型结构并不适用。(2)纤维锌矿型晶体的X3332ω系数可表示成两项之和:单重态(Γ1,Γ3)的贡献和双重态(Γ5,Γ6)的贡献。其中单重态对倍频系数贡献正值,双重态贡献负值。(3)使用Pauling的离子性标度fi来表征A—B键的离子性是适宜的。
关键词: 相似文献
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M. N. Palatnikov V. A. Sandler N. V. Sidorov A. V. Gur’yanov V. T. Kalinnikov 《Physics of the Solid State》2000,42(8):1499-1507
The lithium niobate single crystals doped with B, Zn, and Gd at a content of 0.002–0.44 wt % have been grown. Their domain structure, static and dynamic piezoelectric properties, dielectric properties, and conductivity are investigated over a wide range of frequencies. The dielectric dispersion associated with the Debye-type relaxation process and considerable anomalies in ?′22(T) and conductivity are revealed in the temperature range ~300–400 K. At these temperatures, the piezoelectric modulus d 33 of the initial polydomain crystals LiNbO3: Gd jumpwise increases up to the values close to those for the undoped single-domain crystal. This increase is accompanied by a substantial change in the etch patterns due to the domain structure of the crystal. The nature of the anomalies observed in LiNbO3 in the above temperature range is discussed. 相似文献
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Optical second harmonic generation (SHG) in the form of Cerenkov radiation from ion-implanted lithium niobate (LiNbO3) channel waveguides is analyzed by directly resolving the wave equations. Useful formula of the SHG efficiency is derived and expressed in terms of waveguide parameters. Numerical examples are plotted for LiNbO3 crystals. The results enable the optimization of waveguide design for efficient second harmonic generation in the Cerenkov configuration. 相似文献