Nd2O3纳米晶谱带特征和光伏响应的研究

利用紫外－可见反射光谱对不同粒径的Ｎｄ２Ｏ３纳米晶进行了光吸收特性研究。对其谱带的认证发现，随着样品粒径的变小，部分ｆ→ｆ跃迁的窄带明显增宽并发生红移；另外，在３００～５５０ｎｍ区的边带显著增强。指认这个边带为Ｏ２ｐ→Ｎｄ４ｆ的荷移跃迁。利用表面光电压谱及场调制表面光电压谱对其光伏响应特性、谱带归属及界面电子行为进行了研究，并借助于电荷转移和带间跃迁的概念解释了Ｎｄ２Ｏ３纳米晶谱图的特征。     

含Ce的水热体系中结构稳定性及变价现象

利用ＸＲＤ、ＩＲ及ＸＰＳ谱研究了含Ｃｅ的水热体系中产物及其经过各种后处理的样品结构稳定性及Ｃｅ离子的价态变化。结果表明，不同的原料导致Ｃｅ离子稳定于不同的价态，如直接形成包括纳米晶在内的ＣｅＯ２及一新相ＣｅＯＨＣＯ３，样品ＣｅＯＨＣＯ３经２ＧＰａ的冷压处理未发生结构转变，经高温焙烧处理得到具有高结晶度的棕红色的ＣｅＯ２，当初始原料为Ｃｅ２（ＳＯ４）３和Ｃｅ（ＮＯ３）３时，产物为ＣｅＯ２；而当初始原     

过渡金属复合氧化物电子组态与表面光伏响应的关系（Ⅰ）：M…

利用表面光电压谱及场诱导表面光电压谱研究了部分过渡金属复合氧化物的电子组态与其光伏响应的关系，结果表明，在过渡金属Ｍ（Ｍ＝Ｃｕ，Ｃｏ，Ｎｉ）铁酸盐系列样品中，开壳层的Ｃｕ和Ｃｏ的电荷转移跃迁具有双激发态的成分，其中含有较强的低能电子跃迁；与它们相比，闭壳层的Ｎｉ和铁酸盐的ＣＴ跃迁则需要较大的能量。     

TiO2纳米粒子膜表面性质的研究

ＴｉＯ_２纳米粒子膜在光催化降解大气和水中的污染物［１］、光电转换［２］、光致变色［３］等方面有广阔的应用前景,近年来受到了科学界的高度重视．研究表明,膜的表面性质对如上应用有着重要影响．本文采用等离子体化学气相沉积法（ＰＥＣＶＤ法）［４］制备了ＴｉＯ２的纳米粒子膜,分别采用ＴｉＣｌ４等离子体或Ｏ２等离子体处理膜表面,获得两种不同表面性质的ＴｉＯ２纳米粒子膜;并利用表面光电压谱（ＳＰＳ）和电场诱导表面光电压谱（ＥＦＩＳＰＳ）技术对膜的表面性质进行具体分析,探讨了其在光催化领域的可能应用．１实验部…     

Er2O3纳米晶光伏特性及谱带解析

纳米做教是介于体相材料和分子或原子之间的新型材料，表现出许多超常的电、热、光、磁及催化的特性，因此引起人们高度的重视［1，2］．目前对其光学、磁学、力学和比热等研究已有大量的报导[3]．但是，对于稀土氧化物纳米材料的合成及性质的研究，尤其对它们的电学性质、电子输运方式和光电行为报导较少.本文利用表面光电压谱（SPS）技术对不同粒径的Er2O3纳米晶进行了表面光伏特性的研究，并结合漫反射吸收光谱对其谱带进行了解析，发现，除f→f跃迁外，在300～550nm区间有一定吸收边带，此带可归属于O2p→Er4f电荷转移跃迁．随着样品…     

ZnO纳米粒子的表面光电压谱和光催化性能

采用焙烧前驱物碱式碳酸锌的方法制备了不同粒径的ZnO纳米粒子，而用粒径 最小的作为光催化剂，通过光还原过程分别得了贵金属质量分数为0.5%和0.75%的 Pd/ZnO或Ag/ZnO复合纳米粒子。利用XRD，TEM，XPS，SPS和EFISPS等测试技术对样 品进行了表征，并通过光催化氧化气相正庚烷评估了样品的光催化活性，考察了微 晶尺寸和贵金属Pd或Ag的沉积对ZnO纳米粒子表面光电压信号以及光催化活性的影 响，探讨了样品表面光电压谱与其光催化活性的关系，说明了可以通过表面光电压 谱的测试来初步地评估纳米粒子的光催化活性。结果表明：随着ZnO纳米微晶尺寸 的减小，其SPS信号强度逐渐变弱，而光催化活性逐渐升高；沉积适量的贵金属Pd 或Ag后，ZnO纳米粒子的SPS信号强度明显下降，而其光催化活性却有所升高。此外 ，对ZnO纳米粒子光催化剂的失活机理进行了分析。     

ZnO纳米粒子的表面光电压谱和光催化性能

采用焙烧前驱物碱式碳酸锌的方法制备了不同粒径的ZnO纳米粒子，而用粒径 最小的作为光催化剂，通过光还原过程分别得了贵金属质量分数为0.5%和0.75%的 Pd/ZnO或Ag/ZnO复合纳米粒子。利用XRD，TEM，XPS，SPS和EFISPS等测试技术对样 品进行了表征，并通过光催化氧化气相正庚烷评估了样品的光催化活性，考察了微 晶尺寸和贵金属Pd或Ag的沉积对ZnO纳米粒子表面光电压信号以及光催化活性的影 响，探讨了样品表面光电压谱与其光催化活性的关系，说明了可以通过表面光电压 谱的测试来初步地评估纳米粒子的光催化活性。结果表明：随着ZnO纳米微晶尺寸 的减小，其SPS信号强度逐渐变弱，而光催化活性逐渐升高；沉积适量的贵金属Pd 或Ag后，ZnO纳米粒子的SPS信号强度明显下降，而其光催化活性却有所升高。此外 ，对ZnO纳米粒子光催化剂的失活机理进行了分析。     

双核铁原子簇体系的CI计算

用ＩＮＤＯ／ＣＩ方法研究了含有Ｆｅ－Ｆｅ键的原子簇体系［Ｆｅ２Ｓ２Ｘ４］＾２－（Ｘ＝Ｃｌ，Ｂｒ，Ｉ）的电子光谱及电子结构，对于这些多谱带体系，谱带波数计算值与实验值符合，在谱带的指认分析中，发现了πｄ＾１→πｄ等新的跃迁方式，对跃迁方式作了解释和分类，并讨论了谱带的电荷转移性质，此外，还对体系的化学键等性质进行了分析。     

TiO2纳米粒子膜的制备,表面态性质和光催化活性

在酸性和碱性条件下,用ＴｉＣｌ４水解法制备了ＴｉＯ２纳米粒子膜催化剂。采用原子力显微镜（ＡＦＭ）,Ｘ射线衍射（ＸＲＤ）,表面光电压谱（ＳＰＳ）和场诱导表面光电压谱（ＥＦＩＳＰＳ）测定了催化剂表面的微结构及能级结构。     

纳米CeO_2/聚苯乙烯杂化材料的制备及表征

用反相胶束微乳液法制备了纳米ＣｅＯ２／聚苯乙烯杂化材料．ＸＲＤ分析表明，纳米ＣｅＯ２／聚苯乙烯杂化材料中，ＣｅＯ２是无定形粒子．ＸＰＳ分析表明，杂化材料并非简单的物理混合，ＣｅＯ２纳米粒子与有机物之间存在着一定强度的化学键．ＦＴＩＲ分析表明，ＣｅＯ２粒子的吸收存在蓝移现象．     

CeO2纳米晶的光电量子尺寸效应

ＣｅＯ_２纳米晶的光电量子尺寸效应王德军，崔毅，李铁津，董相廷，洪广言（吉林大学化学系，长春，１３００２３）（中国科学院长春应用化学研究所，长春）关键词纳米晶，ＣｅＯ_２，表面光伏，量子限域纳米材料结构功能特性的研究有着重要的高科技应用背景［１］，但有...     

Raman spectroscopic study on the solvation of N,N-dimethyl-p-nitroaniline in room-temperature ionic liquids

Electronic absorption spectra and Raman spectra of N,N-dimethyl-p-nitroaniline (DMPNA) have been measured in various fluids from the gaseous-like conditions in supercritical fluids (SCFs) to highly polar room-temperature ionic liquids (RTILs). We found that the S0-S1 absorption band center of DMPNA in RTILs is mostly determined by the molar concentrations of ions. On the other hand, the bandwidth of the absorption spectrum does not follow the expectation from a simple dielectric continuum model. Especially in SCFs, the bandwidth of the absorption spectrum decreases with increasing solvent density, suggesting that the intramolecular reorganization energy is a decreasing function of the solvent density. The Raman shift of the NO2 stretching mode has been proven to be a good indicator of the solvent polarity; i.e., the vibrational frequency of the NO2 stretching mode changes from 1340 cm-1 in mostly nonpolar solvent such as ethane to 1300 cm-1 in water. The linear relationship between the absorption band center and the vibrational frequency of the NO2 mode, which was observed for conventional liquids in a previous paper (Fujisawa, T.; Terazima, M.; Kimura, Y. J. Chem. Phys. 2006, 124, 184503), holds almost well for all fluids including SCFs and RTILs. On the other hand, the vibrational bandwidth does not show a simple relationship with the absorption band center. The vibrational bandwidths in RTILs are generally larger in comparison with those in conventional liquids with similar polarity scales. Among the RTILs we investigated, the vibrational bandwidth loosely correlates with the molecular size of the anion. A similar dependence on the anion size is also observed for the bandwidth of the absorption spectrum. We have also investigated the excitation wavelength dependence of the Raman shift of the NO2 stretching mode in RTILs. The extent of the dependence on the excitation wavelength in all fluids is well correlated with the vibrational bandwidth.     

Growth and Spectral Characteristics of Yb3＋-doped LiGd（MoO4）2 Crystal

The Yb3+-doped LiGd(MoO4)2 crystal with the size up to Φ20×30 mm3 has been grown by Czochralski technique.The polarized room temperature absorption and emission spectra have been investigated.This crystal exhibits a broad absorption band centered at 975 nm with an FWHM of 43 and 59 nm for π-and σ-polarization,respectively,and the corresponding maximal absorption cross-sections are 3.36 and 2.42×10-20 cm2.The emission broadband has an FWHM of 47 and 54 nm for π-and σ-polarization,respectively,with the corresponding emission cross sections of 3.92 and 3.34 × 10-20 cm2 at 1020 nm.The measured fluorescence lifetime is 287 μs.     

Structural and optical characterization of Ag-doped TiO2 nanoparticles prepared by a sol–gel method

Undoped and silver-doped TiO₂ nanoparticles (Ti_1?x Ag _x O₂, where x?=?0.00?C0.10) were synthesized by a sol?Cgel method. The synthesized products were characterized by X-ray diffraction (XRD), particle size analyzer (PSA), scanning electron microscope (SEM), and UV?CVisible spectrophotometer. XRD pattern confirmed the tetragonal structure of synthesized samples. Average crystallite size of synthesized nanoparticles was determined from X-ray line broadening using the Debye?CScherrer formula. The crystallite size was varied from 8 to 33?nm as the calcination temperature was increased from 300 to 800?°C. The incorporation of 3 to 5% Ag⁺ in place of Ti⁴⁺ provoked a decrease in the size of nanocrystals as compared to undoped TiO₂. The SEM micrographs revealed the agglomerated spherical-like morphology of particles. SEM, PSA, and XRD measurements show that the particles size of the powder is in nanoscale. Optical absorption measurements indicated a red shift in the absorption band edge upon silver doping. Direct allowed band gap of undoped and Ag-doped TiO₂ nanoparticles measured by UV?CVis spectrometer were 3.00 and 2.80?eV, respectively, at 500?°C.     

J-complexes of retinol formed within the nanoparticles prepared from microemulsions

Retinol nanoparticles have been obtained by direct precipitation of retinol in the inner water cores of AOT/heptane/water microemulsions. The retinol dissolved in chloroform was injected into the microemulsion. The diameter of the so-obtained nanoparticles was measured using transmission electron microscope pictures where the revelation was made thanks to adsorbed iodine on the nanoparticles. The size is ca 6.0 nm, and it is not dependent either on the size of the water droplets or the concentration of the retinol molecules. This phenomenon is explained by the thermodynamic stabilization of the nanoparticles at a certain size. UV-visible spectra of the nanoparticles show a new band the maximum of which has a bathochromic shift with respect to the absorption band of the retinol monomers. If the bathochromic shift is plotted as a function of the line width, a linear correlation is obtained, the line width is decreasing with increasing shift. This behavior is interpreted as being due to an excitonic transition of a J-complex. Quantum chemical calculations have been carried out to confirm the presence of J-complexes. Taking into account the various possible geometries, the results confirm the presence of J-complexes composed of three head-to-tail molecules on the average.     

Ultrafast electronic relaxation and coherent vibrational oscillation of strongly coupled gold nanoparticle aggregates

We report the first direct observation of the ultrafast electronic relaxation and coherent vibrational oscillation of strongly interacting gold nanoparticle aggregates measured by femtosecond laser spectroscopy. The electronic relaxation, reflected as a fast decay component with a time constant of 1.5-2.5 ps, becomes faster with decreasing pump power, similar to earlier observations of isolated gold nanoparticles. Surprisingly, periodic oscillations have been observed in the transient absorption/bleach signal and have been attributed to the coherent vibrational excitation of the gold nanoparticle aggregates. The oscillation period has been found to depend on the probe wavelength. As the probe wavelength is varied from 720 to 850 nm, the period changes from 37 to 55 ps. This suggests that the broad extended plasmon band (EPB) contains contributions from gold nanoparticle aggregates with different sizes and/or different fractal structures. Each of the different probe wavelengths therefore interrogates one subset of the aggregates with similar size or structure. Interestingly, the observed oscillation period for a given aggregate size determined by dynamic light scattering is longer than that predicted based on a elastic sphere model. One possible explanation is that the actual size of the aggregates is larger than what was observed from dynamic light scattering. An alternative, perhaps more likely, explanation is that the vibration of the aggregates is "softer" than that of hard spherical gold nanoparticles possibly because the longitudinal speed of sound is lower in the aggregates than in bulk gold. Persistent spectral hole burning was performed and yielded a hole in the nanoparticle aggregate's extended plasmon band, further supporting that the near-IR band is composed of absorption subbands from differently sized/structured aggregates.     

Hydrothermal synthesis of single-crystal CeCO3OH and their thermal conversion to CeO2

Hexagonal single-crystalline cerium carbonate hydroxide （CeCO3OH） precursors with dendrite morphologies have been synthesized by a facile hydrothermal method at 180 C using CeCl3-7H2O as the cerium source, triethylenetetramine as both an alkaline and carbon source, with triethylenete- tramine also playing an important role in the formation of the dendrite structure. Polycrystalline ceria （CeO2） have been obtained by calcining the precursor at 500 C for 4 h. Tile morphology of the precursor was partly maintained during the heating process. The optical absorption spectra indicate the CeO2 nano/microstructures have a direct band gap of 2.92 eV, which is lower than values of the bulk powder due to the quantum size effect. The high absorption in the UV region for CeO2 nano/microstructure indicated that this material was expected to be used as UV-blocking materials.     

Spectral image analysis for the absorption bands of the beta-methallyl free radical in the vapor phase

The radicals formed in the flash photolysis of 2-methylbut-1-ene and subsequent reactions have been investigated by kinetic spectroscopy and gas liquid chromatography. Less than 10% of photo products are formed by a molecular made of fission of the excited olefin, and of the radical modes the relative probabilities of band fission, beta(CH):beta(CH):alpha(CC) are 13:1.37:1. The extinction coefficients of beta-methallyl radical measured experimentally for all the absorption bands. The decay of the beta-methallyl radical was second order. The rate constant for the beta-methallyl radical recombination experimentally measured was 2.6+/-0.3 x 10(10) l mol(-1)s(-1) at 295+/-2K. The spectrum image showing the absorption bands was examined by image processing techniques in order to improve the visual experience of each band by localizing to a specific region of interest. Experimental results illustrate how the exact location of absorption bands was clearly extracted from the spectral image and further improvements in the visual detection of absorption bands.     

掺硼p型非晶硅薄膜的制备及光学性能的表征

以高氢稀释的硅烷(Si H4)为反应气体,硼烷(B2H6)为掺杂气体,利用RF-PECVD方法,在玻璃衬底上制备出掺硼的氢化非晶硅(a-Si∶H)薄膜,研究了硼掺杂量对氢化非晶硅(a-Si∶H)薄膜的光学性能的影响.利用NKD-7000 W光学薄膜分析系统测试薄膜的透射谱和反射谱,并利用该系统的软件拟合得出薄膜的折射率、消光系数、吸收系数等光学性能参数,利用Tauc法计算掺硼的非晶硅薄膜的光学带隙.实验结果表明,随着硼掺杂量的增加,掺杂非晶硅薄膜样品在同一波长处的折射率先增大后减小,而且每一样品均随着入射光波长的增加而减小,在波长500 nm处的折射率均达到4.3以上;薄膜的消光系数和吸收系数随着硼掺杂量的增大而增大,在500 nm处的吸收系数可高达1.5×105cm-1.在实验的硼掺杂范围内,光学带隙从1.81 eV变化到1.71 eV.     

油酰吗啉溶剂体系中银铟硒纳米颗粒的形貌可控合成

以绿色环保的油酰吗啉作为硒粉的溶剂,油胺作为表面包覆剂,通过简单的液相法制备了银铟硒纳米颗粒。X射线衍射和透射电子显微镜分析测试显示AgInSe2纳米颗粒属于四方黄铜矿相结构,粒径约为16 nm的六角盘状纳米晶。紫外可见光谱分析表明所制备的AgInSe2纳米颗粒禁带宽度约为1.22 eV。考察了反应时间对AgInSe2纳米颗粒尺寸的影响,发现颗粒的尺寸随着反应时间的延长而逐渐变大。对AgInSe2纳米颗粒的生长机制进行了初步探讨,油胺的选择性吸附及材料的晶体结构被认为是决定纳米颗粒形貌的主要因素。