In掺杂ZnO光学性质的第一性原理研究

采用线性缀加平面波的方法,对In元素掺杂ZnO电子结构和光学性质进行研究.计算结果表明:掺In后价带上部分折叠态增加,禁带宽度变窄.不同量In掺杂ZnO与未掺杂时相比,折射率、反射率及消光系数均有明显变化,介电函数虚部向高能量方向移动,而折射率、反射率、吸收系数、消光系数均向低能量方向移动.从理论上指出了光学性质和电子结构之间的联系.     

Pt掺杂CdS光学性质的第一性原理研究

采用基于密度泛函理论的平面波超软赝势方法分析了CdS和Pt掺杂CdS的几何、电子结构和光学性质,计算结果表明Pt掺杂的CdS结构引入了由Pt贡献的导电载流子,增强了CdS的电导率,另外,费米能级下移进入价带.研究表明,Pt掺杂的CdS结构在费米能级附近出现了杂质能级,这是由Pt的5d态电子所形成;在光学性质上,Pt掺杂的CdS在可见光区的吸收系数比理想CdS高,能量损失峰出现红移现象,可见,Pt掺杂的CdS晶体具有更高的光催化活性.     

有机物掺杂下KDP晶体的光学与热学性质研究

本文以L-酒石酸、L-苯丙氨酸和L-丝氨酸为掺杂有机物,采用“点籽晶法”生长出掺杂浓度均为1 mol;的KDP晶体,并利用XRD、光学透过率、热分析以及红外谱图等手段对掺杂后的KDP晶体进行表征,考察有机物掺杂对KDP晶体光学和热学性质的影响.实验发现,掺杂L-丝氨酸的KDP晶体,晶体的熔点温度有所降低;掺杂L-酒石酸时,晶体光学性质得到改善,熔点温度升高;而掺杂L-苯丙氨酸时,结晶质量提高,光学性质得到改善.     

Ca掺杂MgF2光学性质的第一性原理研究

采用基于密度泛函理论的第一性原理平面波超软赝势方法,计算了Ca掺杂MgF2晶体的几何结构、电子结构以及光学性质.结果表明:适量比例的Ca掺杂导致MgF2晶体禁带宽度变窄.在一定能量范围内,Ca掺杂对MgF2晶体的介电常数和吸收系数有调制作用,吸收系数增加有利于光生电子-空穴对的有效分离,提高了MgF2光催化效率,揭示了Ca掺杂MgF2体系在光催化方面的潜在应用.     

Optical Properties of Thick Zinc Oxide Films Doped with Gallium and Gold

Crystallography Reports - Samples of thick (30–32 µm) films of pure and gallium- and gold-doped zinc oxide obtained by magnetron sputtering using an uncooled target have been...     

非线性光学晶体丁二酸锌的生长研究

本文报道了一种金属有机配位聚合物非线性光学晶体--丁二酸锌Zn(C4H4O4)大尺寸单晶生长.通过恒温蒸发法生长出尺寸为7 mm×8 mm×2 mm 的单晶.测定了它在水中溶解度-温度曲线.通过水溶液红外光谱阐明了不同pH值时溶液中各种粒子的浓度分布.借助红外光谱研究了pH值、温度等对晶体生长的影响.Kurtz粉末倍频效应测定证实了丁二酸锌具有非线性光学性能,其倍频强度是KDP的6.5倍.     

Cu掺杂对ZnO基薄膜光学及磁学性能影响

本文采用脉冲激光沉积(PLD)方法在单晶Si(100)衬底上沿c轴方向生长出单晶ZnCoAlO薄膜,并通过加镀Cu层调节薄膜的光学和磁学特性.采用X射线衍射仪(XRD),光致发光光谱仪,振动样品磁强计(VSM)和霍尔效应仪对薄膜的结构、光学和磁学性能进行了研究.实验表明,样品均具有纤锌矿结构并沿(002)面择优生长.加镀Cu层之后,薄膜紫外发光得到增强,掺杂导致薄膜ZnO晶格能带间隙变宽,并使得近带边激子发光增强.同时发现,在室温下Cu离子对薄膜磁性和电子浓度产生影响,Cu掺杂可以改变薄膜中载流子浓度,并影响原有磁性的双交换机理.     

Ag掺杂ZnO薄膜结构和光学特性研究

采用脉冲激光沉积技术制备出了Ag掺杂的ZnO薄膜.研究了Ag含量、衬底温度及氧压对ZnO结构和光学性能的影响.结果表明:Ag以替位形式存在于ZnO晶格中,Ag掺杂浓度较低时,样品具有高度c轴择优取向.衬底温度越高,薄膜的结晶质量越好,光学带隙越接近纯ZnO的带隙,而其紫外荧光峰在衬底温度为300 ℃时最强.氧压为10 Pa时,薄膜的结晶质量最好,紫外峰最强,其带隙则随氧压的增大呈先变窄后加宽的趋势.     

Growth and Optical Properties of Doped LiTaO3 Single Crystals

Single crystals of lithium tantalate (LiTaO₃) doped with Pr, Nd + Yb and Tm were grown by the Czochralski method. A thermal system with 50 mm diameter iridium crucible and two different afterheaters (active and passive) was checked with respect to temperature distribution in a pulling region. The obtained crystals were up to 20 mm in diameter and up 50 mm in length. Crystals were poled, and the Curie temperature was determined for specimens cut of from different parts of single crystals. The polarized absorption spectra, time resolved emission spectra and emission lifetime of Pr³⁺ doped LiTaO₃ crystals were measured. An intense emission from the ³P₀ level was observed. Optical properties of the Yb³⁺ ions excited by energy transfer from Nd3+ ions have been researched for LiTaO₃:Nd, Yb crystals.     

Photonic Heterostructures with Properties of Ferroelectrics and Light Polarizers

The optical and electro-optical properties of a new type of photonic heterostructure composed of alternating ferroelectric molecular layers and optically anisotropic layers of another material are considered. A numerical simulation of the real prototype of this heterostructure, which can be prepared by the Langmuir—Blodgett method from layers of a ferroelectric copolymer (polyvinylidene fluoride trifluoroethylene) and an azo dye with photoinduced optical anisotropy, has been performed. It is shown that this heterostructure has pronounced polarization optical properties and yields a significant change in the polarization state of light at the photonic band edges in the ranges of the maximum density of photon states. The latter property can be used to obtain an enhanced electro-optic effect at small spectral shifts of the photonic band (the latter can be provided by the piezoelectric effect in ferroelectric layers).     

Investigations on the Optical Properties of Undoped,Fluorine Doped and Antimony Doped Tin Oxide Films

Undoped, fluorine doped and antimony doped tin oxide films are prepared on quartz plates by Spray pyrolysis technique. The films grown at the optimum substrate temperature with different doping levels have been chosen for this study. Optical properties of these films are investigated in the entire UV-Visible -IR region (0.2 - 10 mikrom). The observed absorption edge lies at 3.65 eV for undoped tin oxide and on doping it shifts towards higher energies, which is due to the Moss - Burstein effect. For fluorine doping depending upon the fluorine concentration, the absorption edge lies in the range 3.9 - 4.14 eV and for antimony doping it lies in the range 3.82 - 4.1 eV. In the undoped tin oxide films the direct allowed transition occurs at 4.02 eV and indirect allowed transition occurs at 2.43 eV, whereas for fluorine doped tin oxide and antimony doped tin oxide films, the direct allowed transitions occur in the range 4.18 - 4.28 and 4.13 - 4.22 eV respectively and the indirect allowed transitions occur in the range 2.63 - 2.73 and 2.54 - 2.65 eV respectively. Optical properties near the plasma edge have been analyzed using Drude's theory. The dependence of effective mass on carrier concentration has been explained on the basis of nonparabolicity of the conduction band. The shift in the fermi energy, calculated on the basis of energy dependent effective mass, is consistent with the measured shift in the absorption edge.     

Electro-Optical Properties of LCD Doped with Nanoparticles and with Optical Compensators: Ways for Fast Response

This paper consists of two Parts. In the Part 1, we report the experimental results and considerations of the reduction of operation voltage and response time of narrow-gap TN(NTN)-LCDs embedded with the nanoparticles of hydrophobic Aerosil silica. While, in the Part 2, we give a report of the reduction of response time, especially τ_off for the decay process of optically compensated tunable birefringence (OCTB)-mode LCD.     

The Photorefractive and Photovoltaic Properties of a Composite Based on Ferroelectric Polymer Doped with Carbon Nanotubes

The photorefractive effect is obtained in a composite of a ferroelectric polymer (polyvinylidene fluoride with trifluoroethylene (P(VDF/TrFE)) and single-walled carbon nanotubes (SWCNTs), which serve simultaneously as non-linear optical chromophores and spectral sensitizers to a 1064-nm laser beam. It is established that the presence of internal field in the ferroelectric makes it possible to measure the photorefractive effect in the absence of applied external field. Undoped films of VDF/TrFE copolymer are not photosensitive and do not exhibit the bulk photovoltaic effect (BPE). BPE is observed (along with the photosensitivity) in polarized samples, when carbon nanotubes are introduced into the copolymer.     

不同波长条件KDP晶体的非线性光学性质研究

采用Z扫描方法系统的研究了KDP晶体在不同激光波长条件下的非线性光学性质.当λ=355 nm,功率密度为57.92 GW/cm2和λ=532 nm,功率密度为105.94 GW/cm2时,KDP晶体均呈现强烈的反饱和吸收和自聚焦效应,其非线性吸收系数和非线性折射率分别为6.50×10 -2cm/GW,1.17×10 -2cm/GW和8.02×10 -7cm2/GW,6. 14×10 -7cm2/GW;而在1064 nm波长,功率密度为347.95 GW/cm2时KDP晶体并未表现出明显的非线性性质.结果表明,在短波长的激光作用下,KDP晶体更容易产生非线性效应,双光子吸收是KDP晶体非线性吸收的主要机制.     

Optical Properties of Er Doped Congruent and Stoichiometric LiNbO3 Single Crystals

Erbium doped LiNbO₃ (Er:LiNbO₃) single crystal fibers were grown free of cracks along c‐axis by the micro‐pulling down (μ‐PD) method. We have investigated the up‐conversion property with the change of doped Er₂O₃ concentration and the starting melt composition. An enhancement of green upconversion according host matrix is also observed the stoichiometric LiNbO₃. And, the dependence of the green emission according to Er³⁺ concentration is analyzed. The possible application of the Er³⁺ doped stoichiometric LiNbO₃ single crystal fiber for up‐conversion based optical devices is discussed.     

掺杂C60薄膜的制备及光电特性

在电弧法制备的过程中添加氮气或B2O3粉末,制备了氮、硼替位式掺杂C60.硼掺杂和氮掺杂C60均显示明显的半导体导电特性,且室温电导率比未掺杂C60薄膜提高1～2个量级.用共蒸发的方法制备出了硫掺杂C60薄膜,其电导率～温度曲线中存在一个过渡区,过渡区两侧表现出明显的半导体导电特性,这与掺入C60薄膜中的硫杂质的存在状态有关.其室温电导率比掺杂前提高4个量级,光致发光也明显增强.另外还报道了用离子注入和射频等离子体辅助真空沉积的方法制备掺杂C60薄膜的初步结果.     

紫外非线性光学晶体三硼酸铯的生长和性能

采用泡生法和提拉法生长出三硼酸铯(化学式CsB3O5,简称CBO)晶体,研究了晶体生长工艺条件及晶体生长形态.泡生法生长的CBO晶体的尺寸为40mm×25mm×25mm;生长过程中晶体转速为10～20r/min,降温速率为0.1～0.2℃/d.用提拉法生长出20mm×30mm的CBO晶体;生长过程中液面温度梯度为60℃/cm,提拉速度为8mm/d.在生长过程中Cs2O的挥发速度大于B2O3的挥发速度.CBO单晶的晶面由[011]斜方柱和[010]斜方柱单形组成,属于[011]单形是4个较大的面,属于[101]单形是4个较小的三角形晶面.CBO在紫外波段具有较大的有效非线性光学系数.利用CBO进行Nd∶YAG激光和频获得了高转换率的波长355nm及266nm相干光输出.     

ZTS晶体生长及其非线性光学性质研究

利用水溶液缓慢降温法生长了ZTS晶体,最大尺寸达28×16×14mm3;通过X射线粉末衍射实验,得到了晶体的晶胞参数和空间群;通过粉末倍频实验测定了晶体的非线性光学性质,并与KDP晶体的粉末倍频强度对比, 结果表明ZTS晶体是一种优良的、能够实现相位匹配的非线性光学晶体;用紫外.可见光谱仪测量了晶体的透过光谱,在350～1400mm波长范围内透过率超过80;.