Zn_2SnO_4纳米材料制备及光致发光特性

以ZnO、SnO2和活性炭的混合物为原料,通过碳热还原热蒸发法无催化剂成功制备出Zn2SnO4纳米材料.借助X射线衍射仪(XRD)、拉曼光谱和扫描电子显微镜(SEM)对样品物相和形貌进行了表征,结果显示样品为面心立方结构的Zn2SnO4纳米链状棒,同时含有少量的ZnO物相.利用X射线光电子能谱(XPS)对Zn2SnO4样品表面各元素的化学状态及相互作用方式进行了测试,结果表明:样品中Zn和Sn分别是以+2价和+4价氧化态形式存在,其中Zn2p3/2电子有两个结合能,分别来自ZnO和Zn2SnO4,Zn2SnO4中Sn4+占据不同的格点位置.室温下光致发光谱(PL)结果显示,样品在紫外区域(320-450nm)和可见区域存在很强的发光带,其中紫外区域的宽发光带,经过高斯拟合可分为358和385nm两个发光峰,与同条件下制备得到的纯ZnO纳米材料发光谱比较,确认358nm发光峰是来自于Zn2SnO4的近带边复合发光.     

NaTaO3及NaTaO3∶Bi3+光催化剂的光致发光光谱研究

采用光致发光光谱技术对一系列不同条件下制备的NaTaO3及不同掺杂量的NaTaO3∶Bi3+进行了研究. 结果表明, NaTaO3的发光性质与其制备条件密切相关: 在钠离子不足的条件下合成的样品, 其发光带主要位于515和745 nm左右; 而在钠离子充足条件下合成的样品, 其发光带位于460 nm左右, 随着n(Na)/n(Ta)的降低, 发光带向长波长方向移动; 掺入Bi3+之后, 其发光峰由515 nm移至455 nm, 随着Bi3+掺入量的增加, 455 nm的发光带强度减弱. 515 nm的发光带与替位缺陷TaNa....相关; 745 nm的发光带与VNa`缺陷相关; 而460 nm的发光带与本征TaO6基团相关. 将Bi3+掺入到钽酸钠样品, TaNa....由BiNa..替代, 相应的发光带向高的n(Na)/n(Ta)方向移动, 从而呈现出本征TaO6基团的发光带.     

TiO2对ZnO/ZnS:Eu3+荧光粉发光性能的影响

采用溶胶-凝胶-沉淀法制备ZnO/ZnS/2TiO2:Eu3+荧光粉,并采用X射线衍射(XRD)、红外光谱(IR)、透射电镜(TEM)以及荧光光谱技术对其结构、组成、形貌和发光性能进行表征,探讨其发光机理。结果显示,ZnO/ZnS/2TiO2:Eu3+荧光粉的结构在温度高于600℃时趋于稳定状态,呈不规则结构,由ZnO、TiO2和ZnS构成。IR谱图表明,Ti-O-Ti桥氧键网络结构有利于Eu3+之间的能量传递。荧光光谱分析表明,引入TiO2使Eu3+光谱选律禁阻解除,提高了ZnO/ZnS/2TiO2:Eu3+荧光粉的发光性能,且当nZn(NO3)2:nTiO2=1:2时荧光粉的发光性能最好,612 nm处的5D0→7F2电偶极跃迁为最强发射峰,最佳退火温度为600℃。     

ZnO荧光粉中的紫外发射和绿色发射之间的关系

通过在低氧分压和真空中热处理ZnO粉末, 获得了ZnO荧光粉. ZnO荧光粉有两个发射谱带, 分别位于380 nm(紫外)和510 nm(绿色). 紫外谱带对应于ZnO中的激子发射, 是一个单中心发光过程；绿色谱带是一个复合发光过程, 与ZnO中的本征缺陷相关, 如氧空位、锌空位等. 实验表明, 高密度的激发条件有利于紫外发射, 而低氧分压下的热处理有利于提高绿色发射谱带的强度. 研究结果还表明, 与紫外发射相联系的激子可向与本征缺陷相联系的绿色发光中心传递能量, 这种传递可能是通过激子扩散实现的.     

NaTaO_3及NaTaO_3∶Bi~(3+)光催化剂的光致发光光谱研究

采用光致发光光谱技术对一系列不同条件下制备的NaTaO3及不同掺杂量的NaTaO3∶Bi3 进行了研究.结果表明,NaTaO3的发光性质与其制备条件密切相关在钠离子不足的条件下合成的样品,其发光带主要位于515和745nm左右;而在钠离子充足条件下合成的样品,其发光带位于460nm左右,随着n(Na)/n(Ta)的降低,发光带向长波长方向移动;掺入Bi3 之后,其发光峰由515nm移至455nm,随着Bi3 掺入量的增加,455nm的发光带强度减弱.515nm的发光带与替位缺陷Ta.N.a..相关;745nm的发光带与VN`a缺陷相关;而460nm的发光带与本征TaO6基团相关.将Bi3 掺入到钽酸钠样品,TaN..a..由BiN..a替代,相应的发光带向高的n(Na)/n(Ta)方向移动,从而呈现出本征TaO6基团的发光带.     

不同溶剂下制备B_2O_3/SiO_2纳米复合材料对其室温磷光的影响

本文通过对比不同溶剂制备的B2O3/SiO2纳米复合材料室温磷光光谱,并结合FTIR及XRD的表征结果,研究溶剂对该材料磷光性能的影响。结果表明,不管用何种溶剂制备B2O3/SiO2室温磷光材料,均存在两个磷光发射峰,一个是位于520-540nm之间,该发光可能是与氧化硼有关的二氧化硅杂质缺陷发光,另一个位于470-780nm处,该磷光峰推测是二氧化硅的结构缺陷发光。但是在制备过程中溶剂将影响氧化硼在二氧化硅结构中的掺杂,进而影响其发光中心的相对发光强度。     

SiO2/LaF3:Eu3＋核壳结构发光粒子的制备与表征

采用简单的液相法合成了SiO2/LaF3:Eu3＋核壳结构发光粒子, 并对其结构及发光性能进行了表征. XRD分析表明包覆层LaF3:Eu3＋为立方晶相结构, 红外光谱表明SiO2颗粒表面有柠檬酸的修饰, 电镜照片表明合成了球形的核-壳结构的复合粒子, 包覆层厚度为10～20 nm, 光谱测试表明核-壳复合粒子与纯的LaF3:Eu3＋具有相同的发光性能, 均以589 nm附近的5D0—7F1磁偶极跃迁为最强发射峰, 说明Eu3＋在LaF3基质中占据的格位相同.     

ZnO/Eu~(3+)发光材料的高温固相合成及其发光性能

采用高温固相法制备了ZnO/Eu3+红色长余辉发光材料.应用正交试验设计法(每个因素取3个水平,选用L9(34)正交试验表),以初始亮度为指标,研究了煅烧温度、Eu3+质量分数、敏化剂Li+质量分数、煅烧时间等4个因素对发光性能的影响;利用X射线衍射仪对合成的ZnO/Eu3+发光材料进行了物相分析,应用荧光分光光度计测定了样品的激发光谱和发射光谱,应用照射计测定了样品的发光特性.结果表明,当各个因素在水平范围内变化时,所制备的样品均具有ZnO晶格结构;荧光粉的主激发峰位于365 nm和458 nm处,主发射峰位于480 nm、570 nm和600 nm~640 nm,对应于Eu3+的4f和5d间的激发和发射.所确定的最佳合成条件为:煅烧温度850℃,w(Eu3+)=4%,w(Li+)=2.5%,煅烧时间3 h.     

溶胶—凝胶法制备掺Eu^3＋的SiO2玻璃的结构及发光性能

利用溶胶－凝胶技术制备了掺不同量Eu^3 和不同退火温度下的SiO2凝胶和玻璃,通过在不同退火温度下样品的激光发谱,发射光谱,红外光谱和差热－热重曲线,研究了掺Eu3 的SiO2玻璃材料的结构和发光性能,结果显示,当Eu3 的掺杂量大于1．86％（质量分数）,Eu^3 的发光强度趋于稳定,当样品的退火温度大于300度时,SiO2凝胶玻璃中吸附的水已基本除净,此时显示出Eu^3 的特征发射光谱,谱带位置分别是614,596,577nm,分别归属于^5Do-7F2,5D0-7F1,^5D0-^7F0跃迁,对应的激光发光谱显示6个峰,位置分别是318,362,380,393,412,462nm,说明300－500度是凝胶向玻璃转变的关键温度,而水对Eu^3 的发光有强烈的淬灭作用。     

钯氮共掺杂TiO2的制备与表征及其可见光催化活性

在空气气氛和N₂中热处理表面均匀分散有尿素和氯化钯的纳米管钛酸,制备了两个系列Pd/N共掺杂的TiO₂光催化剂,并对所得样品进行了X射线衍射、透射电镜、X射线光电子能谱、紫外-可见漫反射光谱、荧光光谱和电子自旋共振等表征.结果表明,焙烧气氛对样品的形貌、晶体结构、光谱吸收、生成的氧空位浓度和可见光光催化性能的影响很大,其中在空气气氛中制备的样品光催化性能优于在N₂中制备的样品.在可见光(λ≥420nm)照射下,以丙烯为模型污染物考察了样品的光催化活性,发现在空气中400℃下焙烧的样品具有最佳的可见光催化活性.另外,讨论了Pd/N共掺杂TiO₂光催化剂具有可见光响应的机理,认为掺杂的Pd/N元素和制备过程中生成的氧空位是影响可见光催化性能的重要因素.     

Visible emission characteristics from different defects of ZnS nanocrystals

Various sized ZnS nanocrystals were prepared by treatment under H(2)S atmosphere. Resonance Raman spectra indicate that the electron-phonon coupling increases with increasing the size of ZnS. Surface and interfacial defects are formed during the treatment processes. Blue, green and orange emissions are observed for these ZnS. The blue emission (430 nm) from ZnS without treatment is attributed to surface states. ZnS sintered at 873 K displays orange luminescence (620 nm) while ZnS treated at 1173 K shows green emission (515 nm). The green luminescence is assigned to the electron transfer from sulfur vacancies to interstitial sulfur states, and the orange emission is caused by the recombination between interstitial zinc states and zinc vacancies. The lifetimes of the orange emission are much slower than that of the green luminescence and sensitively dependent on the treatment temperature. Controlling defect formation makes ZnS a potential material for photoelectrical applications.     

Tunable photoluminescent and cathodoluminescent properties of ZnO and ZnO:Zn phosphors

ZnO and ZnO:Zn powder phosphors were prepared by the polyol-method followed by annealing in air and reducing gas, respectively. The samples were characterized by X-ray diffraction (XRD), field emission scanning electron microscopy (FESEM), X-ray photoelectron spectra (XPS), electron paramagnetic resonance (EPR), and photoluminescence (PL) and cathodoluminescence (CL) spectra, respectively. The results indicate that all samples are in agreement with the hexagonal structure of the ZnO phase and the particle sizes are in the range of 1-2 microm. The PL and CL spectra of ZnO powders annealed at 950 degrees C in air consist of a weak ultraviolet emission band (approximately 390 nm) and a broad emission band centered at about 527 nm, exhibiting yellow emission color to the naked eyes. When the sample was reduced at the temperatures from 500 to 1050 degrees C, the yellow emission decreased gradually and disappeared completely at 800 degrees C, whereas the ultraviolet emission band became the strongest. Above this temperature, the green emission ( approximately 500 nm) appeared and increased with increasing of reducing temperatures. According to the EPR results and spectral analysis, the yellow and green emissions may arise from the transitions of photogenerated electron close to the conduction band to the deeply trapped hole in the single negatively charged interstitial oxygen ion (Oi(-)) and the single ionized oxygen vacancy (V.O) centers, respectively.     

Growth and Characterization of [001] ZnO Nanorod Array on ITO Substrate with Electric Field Assisted Nucleation

This paper reports direct growth of [001] ZnO nanorod arrays on ITO substrate from aqueous solution with electric field assisted nucleation, followed with thermal annealing. X-ray diffraction analyses revealed that nanorods have wurtzite crystal structure. The diameter of ZnO nanorods was 60–300 nm and the length was up to 2.5 μm depending on the growth condition. Photoluminescence spectra showed a broad emission band spreading from 500 to 870 nm, which suggests that ZnO nanorods have a high density of oxygen interstitials. Low and nonlinear electrical conductivity of ZnO nanorod array was observed, which was ascribed to non-ohmic contact between top electrode and ZnO nanorods and the low concentration of oxygen vacancies.     

Photomagnetism and photoluminescence (PL) of (Pb-Fe-e(-)) complex in lead magnesium niobate-lead titanate (PMN-PT) crystals containing beta-PbO nanoclusters

We present electron paramagnetic resonance (EPR)--evidence of photomagnetism under the conditions of in situ green laser illumination (photo-EPR) in lead magnesium niobate-lead titanate, Pb(Mg,Nb)O3-PbTiO3 (PMN-PT), containing nanoparticles/wires of orthorhombic beta-PbO as identified by Raman spectroscopy. Photo-EPR studies of the sample containing beta-PbO, brownish red in color, have shown intense line at g=2.00, and its yield increased when produced in the presence of 7.5 kG external magnetic field suggesting the formation of magnetic polaron. This was identified as due to interaction between Fe3+, photoinduced Pb3+ and unpaired electron trapped at oxygen vacancies. The photoinduced growth and decay of magnetic polaron has shown a non-exponential behavior. Photoluminescence (PL) studies were conducted with excitation at 308 nm (XeCl laser) and also at 454.5, 488 and 514.5 nm using Ar+ laser. The excitation with 308 nm gave broad PL centered at 500 and 710 nm the latter being quite prominent in beta-PbO containing crystals, along with cooperative luminescence at 350 nm involving two emitting centers. The excitation with Ar+ laser lines, close to the electronic absorption in samples containing beta-PbO gave richer and sharp PL emission in red region from the constituents of the magnetic polaron and also intense anti-Stokes emission on excitation with 514.5 nm radiation. This appears to be due to phototransfer optically stimulated luminescence (PT-OSL) involving electron-hole recombination at photoinduced magnetic polaron site.     

Preparation of ZnO nanoparticles in a reverse micellar system and their photoluminescence properties

ZnO nanoparticles with spherical morphology and narrow size distribution were obtained by calcination of Zn(OH)2 nanoparticles, which were prepared in a polyethylene glycol mono-4-nonylphenyl ether (NP-5)/cyclohexane reverse micellar system and incorporated into polyurea (PUA) via an in situ polymerization of hexamethylene diisocyanate (HDI). The resulting ZnO nanoparticles demonstrated a near-UV emission and a green emission, the intensity ratio of which depended on calcination conditions. For the nanoparticles studied, the calcination atmosphere influenced remarkably the photoluminescence properties such as intensity ratio of the near-UV emission to green emission, rather than the size, morphology, and crystallinity of the ZnO nanoparticles. The green emission decreased by calcination in O2 flow but increased by calcination in N2 flow, as compared with the case calcined in air flow. This finding suggests that the green emission is enhanced with the increase of the number of oxygen vacancies of the ZnO nanoparticles and thus the photoluminescence properties of the nanoparticles were successfully controlled by the calcination condition, without changing the size and morphology.     

The Origin and Dynamics of Soft X‐Ray‐Excited Optical Luminescence of ZnO

The distinct optical emission from ZnO materials, nanoneedles and microcrystallites synthesized with different sizes and morphologies by a flow deposition technique, is investigated with X‐ray excited optical luminescence (XEOL) and time‐resolved X‐ray excited optical luminescence (TR‐XEOL) from a synchrotron light source at the O K and Zn L_3,2 edges. The innovative use of XEOL, allowing site‐specific chemical information and luminescence information at the same time, is fundamental to provide direct evidence for the different behaviour and the crucial role of bulk and surface defects in the origin of ZnO optical emission, including dynamics. XEOL from highly crystalline ZnO nanoneedles is characterized by a sharp band‐gap emission (～380 nm) and a broad red luminescence (～680 nm) related to surface defects. Luminescence from ZnO microcrystallites is mostly dominated by green emission (～510 nm) associated with defects in the core. TR‐XEOL experiments show considerably faster decay dynamics in nanoneedles compared to microcrystallites for both band‐gap emission and visible luminescence. Herein we make a fundamental step forward correlating for the first time the interplay of size, crystallinity, morphology and excitation energy with luminescence from ZnO materials.     

ZnO纳米片组装的微球和层状集聚体的控制合成及其发光性质

通过锌片与水分别在乙二醇和乙二胺中120 ℃反应12 h,直接在锌片上原位合成出ZnO纳米片组装的微球和层状集聚体。利用X射线粉末衍射、扫描电子显微镜、透射电子显微镜和红外光谱对产物进行了表征和分析。结果表明,在乙二醇中得到的直径为0.3～2 µmZnO微球是由直径为30～50 nm纤锌矿结构的ZnO纳米片通过氢键组装而成;在乙二胺中得到的层状集聚体是由20～30 nm的纤锌矿结构的ZnO纳米片通过氢键组装成尺寸约为450×900 nm纳米片,这些较大尺寸纳米片再通过范德华力组装而成。研究了乙二醇和乙二胺在ZnO微球和层状集聚体形成过程中的作用并提出了可能的生长机理。在波长为300 nm光的激发下,发现ZnO微球和层状集聚体具有发光峰位于397 nm强的紫外光发光、485和520 nm弱的蓝绿光发光,它们分别起源于ZnO宽带隙的激子发射,氧空位与间隙氧之间的跃迁以及表面上离子化氧空位中的电子与价带中光激发的空穴之间的复合。     

Polychrome luminescence and photochromic transformations in anthrone solutions

Polychrome luminescence was observed in the UV irradiation of an aerated anthrone solution in ethanol or isopropanol: the initially blue luminescence of the solution changed to indigo blue and then to green. Simultaneously with the luminescence changes, the colorless solution became yellow. The appearance of green luminescence was preceded by a period during which the solution almost did not luminesce. It was found that the photooxidation of ethanol (isopropanol) with oxygen sensitized by anthrone (KH) occurred during irradiation. Green luminescence appeared at the time when the concentration of dissolved oxygen decreased below a critical value. The green luminescence spectrum with a maximum at 495 nm and a shoulder at ～475 nm was ascribed to the oxonium form of anthrone (KH ₂ ⁺ ). The possibility of using the oxygen quenching of the green fluorescence of anthrone solutions for analytical purposes and the use of the anthrone-sensitized photooxidation of ethanol with oxygen for the deoxygenation of solutions in laboratory practice are discussed.     

ZnO纳米管的光学性质及其对甲基橙降解的光催化活性

以十二烷基硫酸钠为模板剂采用水热法合成了ZnO纳米管,以尿素和ZnSO4为原料制备了ZnO纳米颗粒,并应用透射电镜、x射线衍射、光致发射光谱、拉曼光谱、比表面积测定、傅里叶红外光谱和紫外-可见漫反射光谱等技术对样品进行了表征.结果表明,ZnO纳米管的比表面积较大,在λ≈650nm的可见光波段ZnO纳米管开始出现吸收峰,而ZnO纳米颗粒在可见光波段几乎没有吸收.ZnO纳米管和纳米颗粒在紫外光照射下均对甲基橙有降解作用,其中ZnO纳米管的光催化活性较高.随着催化剂用量的增加和光照时间的延长,甲基橙降解率逐渐提高;甲基橙浓度的增大使甲基橙降解率降低.     

Solution,Solid-State Two Step Synthesis and Optical Properties of ZnO and SnO<Subscript>2</Subscript> Nanoparticles and Their Nanocomposites with SiO<Subscript>2</Subscript>

Nanostructure luminescent ZnO and SnO₂ materials are prepared by a two-step solid-state method based on the solution preparation of the macromolecular precursors ZnCl₂·Chitosan and SnCl₂·Chitosan having different ratios (1:1, 1:5 and 1:10), their pyrolysis under air at 800 °C. The pyrolytic ZnO and SnO₂ nanomaterials show a dependence of the particle size, morphology and luminescent properties with the ratio [metal/polymer] in the MCl₂·Chitosan precursors. Thus, ZnO semiconductor materials exhibit luminescence spectra with several emission at 440 nm corresponds to a radiative transition of an electron from the shallow donor level of oxygen vacancies, and the zinc interstitial, to the valence band. On the other hand, the photoluminescence spectrum of the nanostructured SnO₂ shows an intense blue luminescence at a wavelength of 420 nm which may be attributed to oxygen-related defects that have been introduced during the growth process of the nanoparticles. Additionally, whereas SnO₂ was successfully incorporated into SiO₂ structure (SnO₂//SiO₂) by pyrolysis of solid-state mixtures of the precursors SnCl₂·Chitosan in the presence of SiO₂, the same reaction carried out with ZnCl₂·Chitosan precursors led to a mixture of Zn₂SiO₄ and SiO₂. Thus, this new methodology yields nanostructured semiconductor materials, ZnO and SnO₂, suitable for optoelectronic and sensor solid-state devices.