胞嘧啶Ag电极上的表面增强拉曼光谱

胞嘧啶Ａｇ电极上的表面增强拉曼光谱朱克荣（安徽大学现代实验技术中心合肥２３００３９）曹卓良，陈鹤平，赵华正，龙长应（安徽大学物理系合肥２３００３９）Ｓｕｔｒｆａｃｅ－ＥｎｈａｎｃｅｄＲａｍａｎＳｐｅｃｔｒｏｓｃｏｐｙｏｆＣｙｔｏｓｉｎｅＡｄｓｏｒｂｅ...     

(NH_2CH_2COOH)_2CdCl_2晶体的拉曼光谱的研究

（ＮＨ２ＣＨ２ＣＯＯＨ）２ＣｄＣｌ２晶体的拉曼光谱的研究刘建军吴粤郑吉民扈士芬蓝国祥（南开大学天津３０００７１）ＲａｍａｎＳｐｅｃｔｒａｏｆ（ＮＨ２ＣＨ２ＣＯＯＨ）２ＣｄＣｌ２ＣｒｙｓｔａｌｓＬｉｕＪｉａｎｊｕｎ，ＷｕＹｕｅ，ＺｈｅｎｇＪｉｍｉｎ，Ｈ...     

水杨酸分子NIR－FT－SERS与VIS－SERS的比较研究

水杨酸分子ＮＩＲ－ＦＴ－ＳＥＲＳ与ＶＩＳ－ＳＥＲＳ的比较研究方炎，汪媛，胡凤霞（首都师范大学实验中心，首都师范大学综合所北京１０００３７）ＴｈｅＣｏｍｐａｒｉｓｏｎｏｆＶＩＳ－ＳＥＲＳｔｏＮＩＲ－ＦＴ－ＳＥＲＳｏｆＭｏｌｅｃｕｌｅｓＡｄｓｏｒｂｅｄｏ...     

脂类和极性氨基酸的近红外表面增强拉曼散射研究

脂类和极性氨基酸的近红外表面增强拉曼散射研究张崇起，李勤，林书煌（首都师范大学物理系综合所北京１０００３７）ＴｈｅＮＩＲ－ＦＴ－ＳＥＲＳｏｆＡｒｏｍａｔｉｃａｎｄＵｎｃｈｒｇｅｄｐｏｌａｒＡｍｉｎｏＡｃｉｄＡｄｓｏｒｂｅｄｂｙＳｉｌｖｅｒＣｏｌｌｏｉ...     

金胶体系光吸收谱的研究

金胶体系光吸收谱的研究方炎，王玉贤，陈金昌（首都师范大学实验中心，化学系，物理系北京１０００３７）ＴｈｅＯｐｔｉｃａｌＡｂｓｏｒｐｔｉｏｎＳｔｕｄｙｏｆＡｕｓｏｌａｎｄＡｄｓｏｒｂａｔｅ－ＡｕＳｏｌ￥ＦａｎｇＹａｎ；ＷａｎｇＹｕｘｉａｎａｎｄＣｈｅｎ...     

Raman Spectroscopic Study of Nanophase Titanium Dioxide

ＲａｍａｎＳｐｅｃｔｒｏｓｃｏｐｉｃＳｔｕｄｙｏｆＮａｎｏｐｈａｓｅＴｉｔａｎｌｕｍＤｉｏｘｉｄｅＰｅｉＦｅｉ￣＋；ＨｕａｎｇＱｉａｎｇａｎｄＺｈａｎｇＭｉｎｇ一Ｓｈｅｎｇ（ＰｈｙｓｉｃｓＤｅｐａｒｔｍｅｎｔ￣＋，ＣｏｍｐｕｔｅｒＣｅｎｔｅｒ，Ｃｅｎ...     

交流偏置的高T_cdcSQUID的1／f噪声

我们把交流偏置反转技术应用于ｄｃＳＱＵＩＤｓ，观察了各级波形，测出了在交流偏置和直流偏置两种情况下ＹＢＣＯ双品结ｄｃＳＱＵＩＤｓ磁通噪声功率谱密度曲线．交流偏置使１／ｆ噪声显著降低，在ＳＨｚ下的磁通噪声功率谱密度由１×１０－６Φ２０／Ｈｚ降到了３×１０－８Φ２０／Ｈｚ．     

The Squeezing Operator and the Squeezed States of "Superspace

ＴｈｅＳｑｕｅｅｚｉｎｇＯｐｅｒａｔｏｒａｎｄｔｈｅＳｑｕｅｅｚｅｄＳｔａｔｅｓｏｆ＂Ｓｕｐｅｒｓｐａｃｅ＂￥ＳＵＮＣｈａｎｇｙｏｕ（ＤｅｐａｒｔｍｅｎｔｏｆＰｈｙｓｉｃｓ，ＨｅｉｈｅＴｅｃｈｅｒ＇ｓＣｏｌｌｅｇｅ，Ｈｅｉｈｅ１６４３００）ＭＡＡｉｑ...     

A Soft X-ray Streak Camera with Slit Length of 30 mm

ＡＳｏｆｔＸ┐ｒａｙＳｔｒｅａｋＣａｍｅｒａｗｉｔｈＳｌｉｔＬｅｎｇｔｈｏｆ３０ｍｍＱＵＪｕｎｌｅＮＩＵＨａｎｂｅｎ（ＸｉａｎＩｎｓｔｉｔｕｔｅｏｆＯｐｔｉｃｓａｎｄＰｒｅｃｉｓｉｏｎＭｅｃｈａｎｉｃｓ，ＣｈｉｎｅｓｅＡｃａｄｅｍｙｏｆＳｃｉｅｎｃ...     

Time－dependentTheoryofRamanScatteringwithPulses－－ApplicationtoContinuumRamanSpectroscopy

Ｔｉｍｅ－ｄｅｐｅｎｄｅｎｔＴｈｅｏｒｙｏｆＲａｍａｎＳｃａｔｔｅｒｉｎｇｗｉｔｈＰｕｌｓｅｓ－－ＡｐｐｌｉｃａｔｉｏｎｔｏＣｏｎｔｉｎｕｕｍＲａｍａｎＳｐｅｃｔｒｏｓｃｏｐｙＳｏｏ－Ｙ．Ｌｅｅ（ＤｅｐａｒｔｍｅｎｔｏｆＣｈｅｍｉｓｔｒｙ，Ｆａｃｕｌ...     

Nanostructured CdS/CdSSe glass composite for photonic application

The present work describes the synthesis of CdS/CdSSe glass nanocomposites and its characterization. A few glass compositions were optimized and the optimized host glass was remelted along with different semiconductors like CdS and CdSSe at high temperature. The CdS/CdSSe is present in amorphous state in the glass matrix. The thermal treatments have been carefully optimized to obtain well-defined uniform crystal growth of CdS and CdSSe. The glasses with optimized conditions were fabricated and characterized thoroughly using UV, TG/DTA and TEM. The shift in absorption edge to the longer wavelength with heat treatment implies the increase in the crystal size. The band gap has been increased with decrease in the particle size. Crystal size of semiconductors obtained by TEM was 2.5-5 nm for the glass showing absorption edge cut-off at 475 nm (CM-475).     

用近简并三波混频研究半导体掺杂玻璃的非谐振三阶非线性

用近简并三波混频实验方法对半导体CdS_0.4Se_0.6掺杂玻璃在非谐振透明区的三阶光学非线性进行了研究.该实验消除了由于双光子吸收光生载流子的非线性折射产生的五阶非线性效应,仅获得速度快的三阶光学非线性响应.研究结果表明,在非谐振透明区,CdS_0.4Se_0.6掺杂玻璃的三阶非线性极化率并不比它的基底玻璃大很多.量子尺寸效应没有有意义地提高掺杂玻璃中CdS_0.4Se_0.6微晶的三阶非线性极化率,即使较小激子吸收峰的出现也没有发现明显的变化.     

采用紫外光照法在磷酸盐玻璃中合成CdS/Ag复合微粒

掺杂有Ⅱ-Ⅵ族半导体纳米颗粒(如CdS)或者过渡金属(如Ag)的玻璃由于其较大的非线性光学效应而引起人们的极大兴趣,而同时掺杂有半导体/金属的复合微粒则可以进一步增强玻璃的三阶非线性效应,因此成为目前的研究热点。我们利用玻璃沉淀技术及随后的热处理和紫外光还原技术制备了含高浓度(1%)Ag微粒的玻璃,并采用X射线衍射分析了其物相,用高分辨扫描电镜分析了其形貌,以及测试了其吸收和发光性能。从CdS/Ag复合微粒的扫描照片可以发现晶粒均匀分布在玻璃中,尺寸约为1μm。X射线衍射发现经过热处理和紫外光照的样品衍射峰中含有CdS和Ag,而只进行热处理的样品则只含有CdS,未处理的样品则显非晶态。CdS/Ag复合微粒的吸收峰呈现典型的表面等离子共振峰(420nm)以及CdS的峰(600nm),只含有CdS微粒的样品的吸收峰则在480nm附近,未处理的样品在320nm附近有一个吸收峰,这可能是由于样品在快速冷却过程中的微小晶化造成的。只含有CdS微粒的样品有三个明显的发光峰,然而CdS/Ag复合微粒的发过峰则消失。我们提出了共振能量转移机制来解释该现象。讨论了紫外光照还原Ag微粒的机制。可以认为通过紫外光照,CdS表面的电子被激发出来还原Ag+,从而形成银颗粒,伴随着空穴则被表面缺陷所捕获。     

Luminescence of CdS:Ag Quantum Dots in a Polymethacrylate Matrix

Semiconductor quantum dots (QDs) exhibit intense luminescence and reproduce optical characteristics. Doping with metal ions has a positive effect on their properties. Introduction of QDs into polymer matrices leads to the formation of a required morphology of composites. There is a problem in synthesis of optically transparent polymer composites containing QDs of the А²В⁶ group that consists in the extremely low solubility of metal chalcogenides and most of their precursors in monomers. To solve this problem, we used colloidal synthesis. CdS QDs were synthesized by the method of appearing reagents in situ in methylmethacrylate (MMA). Doping with Ag⁺ ions was performed by adding a silver salt into the reaction mixture during the synthesis of CdS QDs. The PMMA/CdS:Ag luminescent polymer glasses were synthesized by radical block polymerization of MMA. The transparency of the composites at wavelengths exceeding 500 nm reaches 92% (5 mm). The luminescence excitation is related to the interband electron transitions in CdS crystals. Luminescence in the range of 500–600 nm is observed due to electron relaxation via a system of levels in the band gap of doped CdS crystals. The positions and intensities of the spectral bands depend on the Ag⁺ concentration, particle size, excitation wavelength, and other factors. The formation of Cd(Ag)S/Ag₂S structures at Ag⁺ concentrations higher than 5.0 × 10^–3 mol/L quenches the luminescence.     

Second-order non-linear optical studies on CdS microcrystallite-doped alkali borosilicate glasses

CdS microcrystal-doped alkali borosilicate glasses were prepared by conventional fusion and heat-treatment method. Utilizing Maker fringe method, second-harmonic generation (SHG) was both observed from CdS-doped glasses before and after certain thermal/electrical poling. While because the direction of polarization axes of CdS crystals formed in the samples is random or insufficient interferences of generated SH waves occur, the fringe patterns obtained in samples without poling treatments showed no fine structures. For the poled samples, larger SH intensity has been obtained than that of the samples without any poling treatments. It was considered that the increase of an amount of hexagonal CdS in the anode surface layer caused by the applied dc field increased the SH intensity. The second-order non-linearity χ⁽²⁾ was estimated to be 1.23 pm/V for the sample poled with 2.5 kV at 360 °C for 30 min.     

Ge-Ga-Cd硫化物玻璃的超快三阶非线性光学性质与结构关系研究

本文采用飞秒时间分辨光学克尔门技术测量了GeS2-Ga2S3-CdS硫化物玻璃体系的超快三阶非线性光学响应，所用激光波长分别为820nm和640nm。?实验结果证明了GeS2-Ga2S3-CdS组分玻璃具有很大的飞秒超快三阶非线性光学响应，另外，其Kerr信号随摩尔组分的不同呈显著变化。通过拉曼光谱结构分析，探讨了此系列硫化物玻璃的三阶非线性光学性质与结构的关系，结果表明构成玻璃网络的四面体结构单元[GeS4]([GaS4])对其超快三阶光学非线性起重要作用。实验还表明了此硫化物玻璃体系的超快三阶非线性不符合半经验的Miller定律。     

化学水浴法和磁控溅射法制备硫化镉薄膜的性能研究

以氯化铵、氯化镉、氢氧化钾和硫脲为反应物采用化学水浴法制备了硫化镉薄膜,为了作对比研究,采用射频磁控溅射以硫化镉为靶材,氩气为溅射气体,制备了硫化镉薄膜。采用X射线衍射、扫描电子显微镜和紫外-可见光光谱仪分别表征了硫化镉薄膜的结构、形貌和光学吸收特性。结果表明,采用以上两种方法制备的硫化镉均具有(002)择优取向,溅射法制备的硫化镉薄膜较致密,薄膜表面较光滑,平均晶粒尺寸在20～30nm;水浴法制备的硫化镉薄膜颗粒尺寸较小,缺陷较多。除了在短波段溅射所得硫化镉薄膜的透过率略差于水浴法所得硫化镉薄膜之外,溅射法制备的硫化镉薄膜的性能整体上优于水浴法制备的薄膜。两种方法制备的硫化镉薄膜的能隙在2.3～2.5eV。     

CdS半导体超微粒子的光学性质

本文研究了水溶胶中的CdS半导体超微粒子和有机溶胶中的粒子表面被有机分子化学修饰的CdS超微粒子的光学性质.我们观察到,当粒子尺寸小于5nm时,CdS超微粒子表现出明显的尺寸量子化效应,并指出CdS超微粒子的表面修饰,增强了它们的发光强度,显著地影响了它们的光学性质。     

ZnS/CdS复合窗口层对CdTe太阳能电池短波光谱响应的影响

采用磁控溅射法制备了ZnS/CdS复合窗口层,并将其应用于CdTe太阳能电池。对所制备薄膜的形貌和结构等进行了研究。测试了具有不同窗口层的CdTe太阳电池的量子效率和光Ⅰ-Ⅴ特性,分析了ZnS薄膜制备条件对CdTe电池器件性能影响;研究了CdS薄膜厚度和ZnS/CdS复合窗口层对短波区透过率以及CdTe太阳电池的光谱响应的影响。着重研究了具有ZnS/CdS复合窗口层的CdTe太阳电池的短波光谱响应。结果表明,CdS窗口层厚度从100 nm减至50 nm后,其对短波区光子透过率平均提高了18.3%,CdTe太阳电池短波区光谱响应平均提高了27.6%。衬底温度250 ℃条件下制备的ZnS晶粒尺寸小于室温下制备的ZnS。具有ZnS/CdS复合窗口层的CdTe电池中,采用衬底温度250 ℃沉积ZnS薄膜来制备窗口层的电池器件,其性能要优于室温下沉积ZnS制备窗口层的电池器件。这说明晶粒尺寸的大小对电子输运有一定影响。在相同厚度CdS的前提下,具有ZnS/CdS复合窗口层的CdTe电池比具有CdS窗口层在短波的光谱响应提高了约2%。这说明ZnS/CdS复合窗口层能够做到减少对短波光子的吸收,从而使更多的光子被CdTe电池的吸收层吸收。     

尺寸相关的CdS纳米颗粒的拉曼散射特性

采用反胶束法,合成了具有不同尺寸的CdS纳米颗粒。利用透射电镜(TEM)和高分辨透射电镜(HR-TEM)以及紫外-可见光吸收谱(UV/vis)对这些纳米颗粒的结构特性进行了表征和分析。利用拉曼光谱仪测量了这些具有不同尺寸的CdS纳米颗粒的拉曼特性。研究结果表明：当纳米颗粒尺寸小于一定值时,拉曼峰出现了蓝移,大于一定值时出现了红移,这些不同的结果是与纳米颗粒的尺寸效应以及纳米颗粒结构中具有各向异性的电子－声子耦合作用有关。