量子尺寸氧化锌颗粒的表面光电压谱研究

氧化锌是极少数几个可以实现量子尺寸效应的氧化物半导体材料[1 ] .传统上 ,这种材料广泛用于陶瓷、压电传感器、催化剂以及发光器件等领域 .随着量子尺寸氧化锌颗粒制备工艺日臻成熟 ,这类材料的应用进一步拓展到光电转换 [2 ] 、光催化[3] 以及化学传感器 [4] 领域 .而在这些领域中的应用都与颗粒的表面性质密切相关 .本工作中制备了两种不同粒径的氧化锌纳米微粒 ,利用表面光电压谱以及电场诱导表面光电压谱对颗粒的表面性质进行了研究 ,并对颗粒的表面态进行了具体指认 .1　实验部分氧化锌纳米微粒参照文献 [5 ,6 ]方法制备 .将 5 .49g…     

钛箔上生长α-Fe2O3纳米氧化膜及其光电性质研究

利用电镀法在钛箔上沉积一层铁镀层,通过热氧化法将铁镀层氧化。利用X射线衍射谱(XRD)、场发射扫描电子显微镜(FESEM)、背散射电子像(BEI)和X射线能量散射谱(EDX)对氧化产物的晶体结构、形貌和组成进行了表征,利用表面光电压谱(SPS)和相位谱(PS)研究了氧化产物的表面光电性质,同时测定了氧化产物的I-V特性。结果表明,铁镀层的表面被热氧化后生成了含α-Fe2O3纳米带和纳米片的纳米氧化膜,α-Fe2O3纳米氧化膜在300～600 nm之间出现了一个与带-带跃迁相关的光伏响应,相位谱显示纳米膜呈n型半导体的导电特征。I-V测试表明在AM 1.5G 100 mW.cm-2标准光强作用下,0.23 V(vs.Ag/AgCl)的偏压下能产生的电流密度为0.58 mA.cm-2。     

TiO2纳米粒子的光催化活性与光伏响应特性研究

TiO2纳米粒子由于其具有良好的化学稳定性、耐光腐蚀性、宽带隙能和大的比表面积等特点而被广泛地应用到光催化降解有机污染物^[1,2]和光催化储能等方面。由于研究手段和研究方法的限制,详细了解催化剂表面光生电荷行为、光谱谱带与催化活性的关系比较困难,而这些关系将为制备高催化活性的光催化剂提供理论基础,由于光催化活性的高低与催化剂的表面性质直接相关,表面光电压谱（SPS）是研究固体材料表面物性和界面间电荷转移过程的有利手段^[3],其为控制光催化机理提供了新的手段。本文利用表面光电压谱方法对系纳米TiO2光催化剂进行了光伏响应测试,发现TiO2的晶型、粒径及表面吸附物对其光催化活性有很大影响。不同性质的表面吸附物可使催化剂表面呈现不同的导电特性,而使其光催化活性不同。利用能带理论和场效应原理对此进行了 合理的解释。     

TiO2单晶的表面光电压谱研究

TiO2由于其优异的光电性质及高的化学稳定性而受到广泛关注,并且被应用于有机污染物光降解[1]、太阳能光电转换[2]等诸多领域.由于制备方法不同,TiO2往往会呈现出不同的光电性质,尽管其晶型与粒度可能相差甚微[3].近年来研究表明,除晶型、粒度等因素外,表面原子排布在决定材料光电性质方面同样有重要贡献[4,5].本文采用表面光电压谱(SPS)及场诱导表面光电压谱(EFSPS)研究了TiO2单晶(001)面的光伏响应.     

有机化合物表面光电压谱的研究

<正> 半导体与金属接触处产生表面势垒,当光照射在样品与金属的接触界面上时,在光照面和非光照面之间建立起电位差,记录这个电位差和入射光波长的关系得到表面光电压谱。表面光电压谱反映材料的光吸收性质和电子的带-带跃迁,同时又受到光生载流子寿命的影响。应用表面光电压技术已经测量了单晶半导体的光伏效应,少数载流子的扩散长度以及表面态等。近来,王德军等用表面光电压谱的方法研究了无机半导体粉末光催化剂的活性。     

Pd/ZnO和Ag/ZnO复合纳米粒子的SPS和XPS研究

用焙烧前驱物碱式碳酸锌的方法制备了ZnO纳米粒子，采用光还原沉积贵金属的方法分别得到了质量分数为0.5％的Pd/ZnO和Ag/ZnO复合纳米粒子，并利用XRD、TEM、XPS和SPS等测试技术对样品进行表征.初步探讨了贵金属在ZnO纳米粒子表面形成原子簇的原因及沉积贵金属对ZnO纳米粒子表面光电压信号的影响.以光催化氧化气相正庚烷为模型反应，考察了沉积贵金属对ZnO纳米粒子光催化活性的影响，并探讨了光催化活性有所提高的内在原因.结果表明， ZnO纳米粒子沉积贵金属后，其表面光电压信号明显下降，而光催化活性却大大地提高，这说明可以通过表面光电压谱的测试来初步的评估纳米粒子的光催化活性，即粒子的表面光电压信号越弱，其光催化活性越高.     

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.对催化剂进行了光催化降解苯酚实验,测定了其光催化活性.结果表明,酸性条件下制备的TiO2膜催化剂的光催化活性较高,其结果接近于P25.用能带理论解释了TiO2纳米粒子膜催化剂光催化活性的差异,分析了膜厚对光催化活性的影响.     

纳米晶钛酸铅表面态对介电性能的影响

将醋酸铅、钛酸四丁酯和硬脂酸在熔融状态下混合均匀后置于冷水浴中，使其凝固成凝胶，经不同温度焙烧，制成纳米晶PbTiO3.用X射线衍射光谱、红外光谱对产物进行表征.采用X射线光电子能谱和表面光电压谱对纳米晶PbTiO3表面状态分析,发现材料表面的不完整性主要是由氧空位造成.暴露在粒子表面的主要是金属离子.随着晶粒尺寸的减小，材料表面氧空位缺陷浓度增加，表面光伏效应增强，谱带变宽.纳米晶PbTiO3材料的表面状态对其极化性质有着重要的影响，使其静态介电常数远大于常规材料的静态介电常数.     

纳米Hg2Cl2/Al2O3有序阵列体系的制备和表征

纳米结构材料由于其独特的物理化学性质以及在微电子器件、光开关等方面的应用而备受关注. 多孔氧化铝由于具有孔径分布较窄、取向一致和孔密度高等优点而广泛用于模板制备纳米结构材料. 在多孔氧化铝中可以组装金属纳米粒子[1]、半导体纳米粒子[2]、导电高分子[3]以及碳纳米管[4]等.     

利用水相合成的量子点标记木瓜蛋白酶的研究

利用半导体纳米粒子 (也称半导体量子点 ,Quantum Dots,以下简称 QDs)和表面修饰技术制备的半导体荧光探针具有极其优良的光谱特征和光化学稳定性 [1] .自 1 997年以来 ,随着量子点制备技术的不断提高 ,量子点在生物医学方面已有应用 . 1 998年 ,Alivisatos[1] 和 Nie[2 ] 两个研究小组分别将结合了生物分子的 QDs作为荧光探针应用于生物体系 ,开创了纳米粒子应用的新领域 .最近 Nie等 [3 ]在利用量子点编码生物分子的研究中取得了突破性进展 .目前 ,纳米粒子与生物分子的连接以共价键方式相结合最为常见 [1,2 ,4 ,5] ,而且在这些应用中…     

TiO2纳米带表面光伏特性的研究

近年来, 一维结构的纳米带由于其不同于管、线材料的新颖结构以及独特的光电性能而受到广泛关注. 人们通过各种方法合成了氧化锌、硫化镉和氧化锡等纳米带材料[1,2]. 纳米TiO2以其优异的光电性能和高的化学稳定性而被广泛应用于太阳能电池、光催化降解等诸多领域[3], 从而成为研究热点, 最近其纳米带的制备也有报道[4].     

四甲基-四乙基钯卟啉的表面光伏特性研究

合成了1,3,5,7－四甲基－2,4,6,8－四乙基卟啉（TMTEP）及其钯络合物（PdTMTEP),并利用表面光电压谱（SPS）和场诱导表面光电压谱（FISPS）技术对它们的表面光伏特性进行了研究。TETEP有较强的荧光发射,而PdTMTEP以磷光辐射为主,其光伏响应强度比TMTEP的强得多;在外电场诱导下,PdTMTEP的Soret带与Q带的光伏响应强度随外加正电场光伏响应强度的增加而增强,随外加负电场光伏响应强度的增加而减弱,并且在680,750nm处出现两个新的光伏响应带,这两个光伏响应带与极化子跃迁有关。     

Synthesis of ZnO nanorods and their application in quantum dot sensitized solar cells

ZnO nanorod thin films of different thicknesses and CdS quantum dots have been prepared by chemical method. X-ray diffraction pattern reveals that the CdS quantum dot and ZnO nanorods are of hexagonal structure. Field emission scanning electron microscope images show that the diameter of hexagonal shaped ZnO nanorods ranges from 110 to 200 nm and the length of the nanorod vary from 1.3 to 4.7 μm. CdS quantum dots with average size of 4 nm have been deposited onto ZnO nanorod surface using successive ionic layer adsorption and reaction method and the assembly of CdS quantum dot with ZnO nanorod has been used as photo-electrode in quantum dot sensitized solar cells. The efficiency of the fabricated CdS quantum dot-sensitized ZnO nanorod-based solar cell is 1.10 % and is the best efficiency reported so far for this type of solar cells.     

Physicochemical Interaction of ZnO Fine Particles with 5‐Mono‐(4‐carboxyphenyl)‐10,15,20‐Triphenylporphyrin

This study deals with an investigation on the preparation and physicochemical interactions of ZnO nanoparticles with acid functionalized porphyrin [5‐mono‐(4‐carboxyphenyl)‐10,15,20‐triphenylporphyrin (CPTPP)] for photovoltaic applications in a detailed manner. Zinc acetate and sodium hydroxide were used as the starting materials for the synthesis of ZnO nanoparticles at 60 °C in an alcoholic medium. The freshly prepared fine particles were then functionalized with CPTPP. Both the virgin and pregnant ZnO particles were characterized by using UV‐Visible spectrophotometry (UV), fluorescence emission (PL), Fourier transform infrared spectroscopy (FTIR), X‐ray diffraction (XRD) and scanning electron microscopy (SEM). The band gap energy obtained for ZnO particles, having a value of 3.47 eV, shows significant quantum confinement effect and enhanced photophysical activity. FTIR analysis of the doped ZnO nanostructures showed the presences of some chemical species. SEM analysis revealed a clear change in the surface morphologies of undoped ZnO. The average crystallite size of nanoparticles, calculated from XRD peaks, was found in the nano regime. The lattice parameters calculated for ZnO nanocrystals were also found in good agreement with those given in the literature. From the enhancement in the red shift of the UV‐Vis spectra, it is concluded that hybridization of acid functionalized porphyrin can cause a significant expansion in the total absorption region of ZnO semiconductor for photovoltaic applications.     

ZnO/Cu2O异质结中深能级表面光伏特性

采用恒电压沉积法在导电玻璃(FTO)上制备了具有三棱柱金字塔状的ZnO/Cu2O异质结薄膜. 利用场发射扫描电镜(FESEM)与X射线衍射仪(XRD)对薄膜的微观形貌和晶体结构进行了表征. 利用表面光电压谱(SPS)、场诱导表面光电压谱(FISPS)和相位谱(PS)研究了单一Cu2O与ZnO/Cu2O异质结薄膜的表面光伏性质. 结果表明, 与单一Cu2O薄膜相比, ZnO/Cu2O异质结薄膜的光伏响应范围拓展到了600~800 nm. 根据SPS, FISPS和PS的作用原理, 拓展部分的光伏响应归因于ZnO/Cu2O异质结中Cu2O层的深能级跃迁, 该跃迁在ZnO-Cu2O界面电场(方向由ZnO指向Cu2O)的作用下得到加强, 同时深能级跃迁产生的电子-空穴对在ZnO-Cu2O界面电场的作用下得到了有效分离和传输.     

Optical properties of zinc oxide nanoparticles and nanorods synthesized using an organometallic method.

The emission properties of nanocrystalline ZnO particles prepared following an organometallic synthetic method are investigated. Spherical particles and nanorods are studied. The shape of the particles and the ligands used are shown to influence the luminescence properties in the visible domain. Two different emissions are observed at 440 nm (approximately 2.82 eV) and at 580 nm (approximately 2.14 eV) that are associated with the presence of surface defects on the particles. The first emission corresponds to the well-known yellow emission located at 580 nm (approximately 2.14 eV) with a lifetime of 1850 ns for 4.0 nm size ZnO nanoparticles. The second emission at 440 nm (approximately 2.82 eV) is observed when amine functions are present. This strong blue emission is associated with an excitation energy less than that associated with the yellow emission displaying a lifetime of nine nanoseconds. A possible hole trapping effect by the amine groups on the surface of the ZnO particles is discussed as the origin of this emission. The modification of the intensities between the two visible emissions for different particle shapes is proposed to be related to a specific location of the amine ligands on the surface of the particles.     

Fabrication and photoluminescent properties of heteroepitaxial ZnO/Zn0.8Mg0.2O coaxial nanorod heterostructures

ZnO/Zn0.8Mg0.2O coaxial nanorod heterostructures were prepared by employing catalyst-free metal-organic vapor-phase epitaxy, and their structural and photoluminescent (PL) properties were investigated using transmission electron microscopy (TEM) and temperature-dependent PL spectroscopy. TEM images show that ZnO/Zn0.8Mg0.2O layers were epitaxially grown on the entire surfaces of the ZnO nanorods and the ZnO nanorod diameters as a core material were as small as 9 +/- 2 nm. A dominant PL peak was observed at 3.316 eV, from room-temperature PL spectra of ZnO/Zn0.8Mg0.2O coaxial nanorod heterostructures with ZnO core diameters of 9 nm, indicating a PL blue shift of 30 meV, which resulted from a quantum confinement effect along the radial direction in ZnO nanorods. Furthermore, temperature-dependent PL properties of the coaxial nanorod heterostructures were investigated, showing much higher PL intensity for the coaxial nanorod heterostructures than that of bare ZnO nanorods at room temperature. The origin of the enhanced PL intensity and reduced thermal quenching for the coaxial nanorod heterostructures is also discussed.     

活性粒子吸附对ZnO纳米粒子表面光伏特性的影响

作为一种传统的半导体,氧化锌在压电陶瓷、光电化学、光催化、发光器件以及气体传感器等方面具有广阔的应用前景,特别是氧化锌纳米粒子,由于其比表面积大、表面活性较高和对周围环境的敏感性,使其成为传感器研究领域中最有前途的材料,有关生物氧传感器和激光器的光电功能特性以及其能带结构的研究已有报道,     

Synthesis and characterization of PbS nanorods in W/O microemulsion system

PbS nanorods have been successfully synthesized in water-in-oil (W/O) microemulsion containing non-ionic surfactant OP, n-pentanol, cyclohexane, and aqueous solution. The effects of the molar ratio of water to surfactant (ω₀), the concentration of reactants and the ageing time on the morphologies of PbS nanoparticles were investigated. The microstructures, morphologies and properties of the synthesized products were characterized by means of X-ray diffraction, transmission electron microscopy, and ultraviolet-visible (UV-VIS) absorption spectroscopy, respectively. The results showed that the synthesized rod-like products are composed of cubic phase PbS. These nanorods have an average diameter of about 100 nm, and an average length of about 500 nm. In the UV-VIS absorption spectrum, the absorption edge of PbS nanorods exhibit a blue shift compared with that of bulk PbS, indicating the quantum confinement effect of PbS nano-particles