共查询到19条相似文献,搜索用时 187 毫秒
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合成了大螺旋扭曲力的手性化合物4,4′-2(戊基-环己基)苯甲酸异山梨醇酯(ISBB)。对60.0μm厚ISBB/液晶性单体/向列相液晶/光引发剂复合体系的液晶层的上、下表面温度施加不同温度,液晶层中形成了温度梯度。由于高温区域的液晶溶解ISBB的能力强,低温区域的ISBB会向高温区域扩散,从而在液晶薄层中形成了ISBB的浓度梯度与螺距梯度。紫外光聚合复合体系中的光可聚合单体,单体间交联聚合形成网络固定住了液晶层内的螺距梯度,从而制备出反射可见光波段的右旋圆偏振光的宽波反射液晶薄膜。 相似文献
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采用手性剂掺杂向列相混合液晶制备出具备类似胆甾相液晶温变显色性能的液晶混合物。通过控制向列相液晶中手性剂的添加量,调节混合液晶的颜色,制备出系列室温下呈颜色转变的液晶混合物。在此基础上,探究3种不同添加剂对混合液晶显色性能的影响,确定具备最佳温变显色性能的液晶混合物配方。以上述液晶混合物为芯材、异佛尔酮二异氰酸酯(IPDI)为壁材,采用界面聚合法在不同反应条件下制备出一系列液晶微胶囊,并确定最佳反应条件。结果表明:最佳反应条件下,制备的液晶微胶囊粒径范围在50~105μm之间,平均粒径在68.06μm左右,囊芯材料含量约占35%。液晶微胶囊呈规则球形,粒径比较均匀,具有良好的温变显色性能,且热稳定性较高,热分解温度达330℃以上。 相似文献
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介绍了双向反射分布函数的测量原理和方法,搭建了双向反射分布函数的测量装置。该装置可以测量可见光和红外两个波段的双向反射分布函数。在可见光波段采用卤钨灯作为光源,采用光纤光谱仪作为光接收器,以10 nm的波长间隔测量双向反射分布函数。在红外波段采用碳化硅作为红外光源,采用热释电探测器作为光接收器,采用标准板相对定标的方法测量待测样板的双向反射分布函数。可见光波段双向反射分布函数的测量重复性不大于1.5%;3μm~5μm红外波段双向反射分布函数的测量重复性分别小于或等于2.5%、8μm~12μm波段的小于或等于3.0%。测量结果表明,该测量装置的有效性较高。 相似文献
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通过偏光显微镜法、紫外-可见光光谱学、XRD和电导率分析方法研究了大功率超声对纤维素纳米晶体(CNC)的溶致胆甾相液晶(N*-LC)螺距的影响及其在干燥状态下所制得薄膜的光学性能。研究结果表明,溶致N*-LC的螺距随着超声功率的增大而增大,其干燥薄膜的反射波波长红移,且红移幅度与超声功率有关。但是,CNC的晶型和尺寸没有明显变化。电导率测试结果表明,超声处理使溶致N*-LC的电导率提高。由此推测溶致N*-LC的螺距增大的主要原因是大功率超声处理使束缚在双电层中的带电离子释放出来,进而CNC粒子之间的静电斥力变大所致。 相似文献
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设计制作染料掺杂聚合物分散液晶薄膜激光器件,研究随机激光辐射行为。利用微胶囊法将激光染料、向列相液晶、手性剂、聚乙烯醇混合,制备掺杂两种激光染料的聚合物分散液晶薄膜。利用输出激光532 nm的Nd:YAG倍频脉冲激光器进行泵浦,在582~607 nm波段获得尖锐、离散的随机激光输出,阈值能量约为9 mJ,线宽约为0.3~0.4 nm。对于器件产生激光辐射的机制,利用环形腔理论进行了分析。对比掺杂单种激光染料的聚合物分散液晶薄膜激光器件,实验结果显示,同时混合不同类型的激光染料制备的聚合物分散液晶薄膜,能够实现较宽波段的随机激光输出。 相似文献
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非直流电压对N*-SmC*相序铁电液晶排列的影响 总被引:1,自引:1,他引:0
半"V"字形铁电液晶器件中使用N* -SmC*相序的铁电液晶材料,获得此种器件单畴排列的常用方法是在N*-SmC*相变过程中施加直流电压,但是这种方法引入了损害器件性能的剩余电荷.通过研究在相变过程中施加各种非直流电压对液晶排列织构的影响,发现直流电压不是得到N*-SmC*相序的铁电液晶均一排列的必要条件,通过选择双极性电压为V1=7V/μm,V2=3 V/μm,一个脉冲周期20 ms内施加双极性电场时间比为D1/D2=3/7,不仅获得了电光特性曲线不存在迟滞回线的均一层排列器件,同时也解决了剩余电荷对器件的影响. 相似文献
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根据超导测辐射热计的理论,以YBCO为材料,制备的高温超导薄膜型红外测辐射热计,黑体响应度Rv>104V/W,D*>1010cmHz1/2W-1,NEP≈10-14WHz-1/2。测量和分析了器件的频率响应、噪声特性和其对1~15μm波段及118.8μm,337μm,570.5μm,699μm,1009.4μm等波长的光谱响应。测量结果表明,高温超导红外测辐射热计对整个红外波谱都有响应,但其性能在远红外波段衰减很厉害,因此,对器件的表面处理应是提高其长波性能的一个关键。 相似文献
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离子束溅射氧化物薄膜的中红外特性 总被引:2,自引:0,他引:2
以离子束溅射沉积(IBSD)方法制备了Al2O3、Nb2O5单层膜,用红外可变角度光谱椭圆偏振仪(IR-VASE)测试了薄膜的光学常数。用原子力显微镜(AFM)测量了单层膜的表面形貌及表面粗糙度,计算了单个表面的总积分散射(TIS)。以Nb2O5和Al2O3为高低折射率材料设计并制备了2.7μm高反射膜。最后对单层膜进行了环境实验检测。结果表明,制备的薄膜在中红外波段具有高的折射率和低的消光系数,光滑的表面特性和极低的表面散射损耗;在2.7μm波段没有发现由于水吸收导致的消光系数的增大;制备的反射膜在2.7μm反射率达到了99.63%,接近于理论计算值。薄膜顺利通过了一系列环境实验,显示其优良的环境稳定性。 相似文献
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Based on the analytical expression of the electromagnetic field solution of a helical symmetric dielectric material, the relationship between spectral reflectivity and birefringence of a chiral liquid crystal and the blue shift of the Bragg reflection in the condition of oblique incidence are presented in this paper. The theoretical results indicated that: 1) If birefringence (An)of the liquid crystal is greater than 0.2 and the thickness of the liquid crystal layer reaches 3μm, the liquid crystal layer will reflect more than 90% of the incident light; 2)To reflect the whole visible spectrum by Bragg reflection,An of the liquid crystals in plane alignment state should exceed 0.6; 3) When the incident beam inclines to 60°from the normal direction, the blue shift of the reflective spectrum will reach to 100 nm. On the other hand, since the An of the commercial chiral liquid crystals is not larger than 0.2, to get the entire visible reflective spectrum, it needs to introduce a polymer network into the liquid crystals and make a sagging structure on the surface of substrates. The contribution of the network is to establish random anchorage that makes the pitch varied, hence broadening the Bragg reflection spectra.The random distribution of the sagging structure on the surface substrate is used to induce random screw axes of the chiral liquid crystal, which not only causes a blue shift of Bragg reflection but also further stretches the reflection spectra. Experiments demonstrated that the Bragg reflection spectrum could be broadened from by introducing both polymer network and sagging structure on the substrate surface cell. 相似文献
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It is shown experimentally that the cell with an n-type nematic liquid crystal may have two functions, light deflection and shutter, and that the cell with a reflective coating film may deflect a light beam about twice the angle achieved with a transmission type of cell. 相似文献
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Iam Choon Khoo Min-Yi Shih Wood M.V. Guenther B.D. Pao Hsu Chen Simoni F. Slussarenko S.S. Francescangeli O. Lucchetti L. 《Proceedings of the IEEE. Institute of Electrical and Electronics Engineers》1999,87(11):1897-1911
The basic mechanisms of photo-induced space charge field formation, director axis re-orientation, and refractive index changes in fullerene C60- and dye-doped nematic liquid crystals films are presented. In particular, in aligned methyl-red-doped nematic liquid crystal film, we observe a nonlinear index change coefficient as high as 10 cm2/W, associated with purely optically induced liquid crystal director axis re-orientation. Experimental observations of dynamic and high-resolution storage holographic grating formation, two beam coupling with gain of nearly 3000 cm-1, optical limiting action at nanowatt cw laser power, and incoherent-coherent image conversion at μW/cm2 light intensity level are discussed 相似文献
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液晶材料对电、热、磁、光等外界物理量的变化具有不同的响应特性,向其中添加具有一定特性的化合物,可以得到具备一定响应特性的液晶复合材料。利用所制备的液晶复合材料对于电场变化具有响应特性的特点,制备出具有信息记录功能的复合材料。合成手性离子液体,按一定配比将其加入手征向列相液晶(N~*-LC)中,得到反射波段可电控的手征向列相液晶/手性离子液体复合材料。实验结果表明:材料初始状态为光透射状态;对材料施加直流电压40V时,样品表现为光散射状态,透过率低于10%;施加高频交流电压40V时,样品表现为半透明镜面反射,反射范围覆盖400~750nm,透射率为45%左右;撤去电场后,可恢复至初始状态,并且每种状态都具有一定的记忆效应。该种液晶复合材料制备简单,无需紫外辐射工艺,且具有电场响应特性,可以通过电场控制在可见光范围内表现出光透射、强烈光散射、半透明镜面反射3种不同状态,具有记忆效应,操作简单方便。 相似文献
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Chiroptical Resolution and Thermal Switching of Chirality in Conjugated Polymer Luminescence via Selective Reflection using a Double‐Layered Cell of Chiral Nematic Liquid Crystal
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An optically resolvable and thermally chiral‐switchable device for circularly polarized luminescence (CPL) is first constructed using a light‐emitting conjugated polymer film and a double‐layered chiral nematic liquid crystal (N*‐LC) cell. The double‐layered N*‐LC cell with opposite handedness at each layer is fabricated by adding each of two types of N*‐LCs into each of the cells, and the N*‐LCs consist of nematic LCs and chiral dopants with opposite chirality and different mole concentrations. The selective reflection band due to the N*‐LC is thermally shifted so that the band wavelength is close to the luminescence band of the racemic conjugated polymer, such as disubstituted polyacetylene (diPA), yielding CPL with opposite handedness and high dissymmetry factor values (|glum|) of 1.1–1.6 at low and high temperatures. The double‐layered N*‐LC cell bearing the temperature‐controlled selective reflection is useful for generating CPLs from racemic fluorescent materials and for allowing thermal chirality‐switching in CPLs, which present new possibilities for optoelectronic and photochemical applications. 相似文献
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Fushan Zhou Deng-Ke Yang 《Display Technology, Journal of》2005,1(2):217-224
In this paper, we studied the optics of transmissive bistable nematic liquid crystal displays by using the Poincare sphere approach. We derived analytical solutions of the polarization state of the outcoming light for the two bistable states. We have found the optimum modes of film compensated bistable twisted nematic liquid crystal displays. Our results show that the number of optimized modes at a fixed wavelength of film-compensated bistable twisted nematic (BTN) is infinite. We identified the optimized modes for displays operated in the whole visible light wavelength region. We calculated the transmission spectra of the two bistable states of the optimized modes. 相似文献
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Fascinating nematic‐ and smectic‐like self‐assembled arrays are observed for gold nanorods partially capped with either laterally or terminally attached nematic liquid crystals upon slow evaporation of an organic solvent on TEM grids. These arrays can be manipulated and reoriented by applying an external magnetic field from quasi‐planar to vertical similar to a Fréedericksz transition of common organic nematic liquid crystals. Birefringence and thin film textures of these self‐assembled gold nanorod arrays observed by polarized optical microscopy are strongly reminiscent of common organic nematic liquid crystal textures between crossed polarizers and, additionally, support the formation of ordered liquid crystal‐like anisotropic superstructures. The ordering within these arrays is also confirmed in bulk samples using small angle X‐ray scattering (SAXS). 相似文献