BaZr1-xAlxO3(x=0～0.08)中空微球的制备与发光性能

采用水热法合成了BaZr1-xAlxO3(x=0~0.08)中空微球,通过XRD,SEM,TEM,PL,FTIR等测试手段对样品进行了表征。XRD结果表明,铝成功地掺杂进入了BaZrO3晶格中,占据了B位ZrO6八面体中Zr4+的位置,铝的掺入导致晶胞参数的减小。TEM结果证实了微球的空心结构,产物的平均粒径为150 nm。中空微球在355 nm激光的激发下,均发出波长为423 nm的紫光。与未掺杂的BaZrO3相比,铝掺杂引起的晶格收缩使发光强度呈整体下降趋势,而不等价掺杂引起的氧空位变化导致发光强度随着铝掺杂量的增加出现先增强后减弱的现象。     

钇掺杂有序大孔TiO_2微球的制备与光催化性能研究

采用溶胶-凝胶法、胶体晶体模板法制备了钇掺杂有序多孔TiO2微球,利用FTIR,SEM,XRD,XPS,UV-V is分析对其进行表征,并研究钇掺杂前后材料的光催化性能。结果表明:钇掺杂有序多孔TiO2微球规整致密,但局部有孔洞的塌陷。钇掺杂前后有序多孔TiO2微球的晶型没有改变,仍为锐钛矿型。XPS分析发现钇掺杂有序多孔TiO2微球是可行的,材料中含有钇元素含量约为1.0%。UV-V is分析表明钇掺杂使得TiO2吸收光红移至可见光区,甲基橙降解实验显示掺钇有序多孔TiO2微球的光催化性能好于未掺钇TiO2的光催化性能。     

以氨基酸为晶体生长控制剂合成多级纳米结构的硫化铟空心微球

以水热方法制备具有多级纳米结构的In2S3空心微球. 通过对不同反应时间产物的跟踪表征, 证明微球中空结构的形成归因于Ostwald ripening机理. 空心微球的壳层由In2S3的纳米粒子或纳米片组成, In2S3空心球的紫外可见光谱蓝移以及荧光光谱在约385 nm的强发射和364 nm的弱发射, 均显示了纳米尺度In2S3晶体的量子局限效应. 以不同的氨基酸作为晶体生长修饰剂, 可以选择性地制备不同表面形貌的In2S3空心微球, 显示了氨基酸的不同功能团在In2S3晶体生长过程中对表面形貌的控制作用.     

中空TiO_2微球的制备及对聚丙烯酸酯薄膜性能的影响

采用阳离子聚苯乙烯微球作为模板,钛酸四丁酯为钛源,氨水为催化剂,制备了中空TiO_2微球.采用X射线衍射、扫描电镜及比表面测定仪对其形貌和结构进行了表征,并考察了模板粒径、钛源用量以及催化剂用量对中空TiO_2微球形貌的影响.通过物理共混法将其引入至聚丙烯酸酯乳液中并成膜,研究了复合薄膜的保温性能、抗紫外性能及力学性能.结果表明,锐钛矿相中空TiO_2微球模板粒径、钛源用量以及催化剂用量影响中空TiO_2微球的空心尺寸、壁厚及壳层致密性.中空TiO_2微球可显著提升聚丙烯酸酯薄膜的保温性能、抗紫外性能和力学性能.采用不同粒径的模板制备的中空TiO_2微球对复合薄膜的各项性能均有影响,其中模板粒径为140 nm时复合薄膜性能最优,光反射率提升63%,导热系数降低27%,且在波长小于360 nm范围内,紫外透过率几乎为0,抗张强度增加100%,断裂伸长率提升62%.     

水热沉淀法制备掺铁二氧化钛中空球及其光催化性能

 以碳球为模板剂, 采用水热沉淀法制备了不同配比掺 Fe 的 TiO2 (Fe-TiO2) 中空球, 并运用 X 射线粉末衍射、扫描电子显微镜、元素分析能谱、红外光谱和热重等方法对其进行了表征. 结果表明, 中空球为锐钛矿相, 大小为 0.5~3.20 ?m, 壳层厚度为 30~60 nm, 比表面积为 150~300 m2/g. 随着 Fe 掺杂量的增加, 中空球在可见光区的吸收强度逐渐增加. 光催化降解实验表明, 掺 Fe 后, TiO2 中空球的可见光催化活性升高, 其中 0.5% Fe-TiO2 在 80 min 内降解亚甲基蓝超过 75%. 同时还讨论了光催化机制.     

可见光响应的铁掺杂TiO_2中空微球的制备及其光催化性能

以聚苯乙烯微球作为模板,水溶性过氧化钛配合物作为前驱体一步合成了掺铁TiO2中空微球,并利用XRD,SEM,TEM,XPS,UV-Vis等测试手段对样品进行了表征。结果表明,一步法制备的掺铁TiO2中空微球以锐钛矿相存在且具有良好的中空结构,掺杂少量铁到体系中,改变了其电子结构,使其吸收波长拓展到可见光区。光催化降解亚甲基蓝溶液的结果表明,掺杂0.75%铁的TiO2中空微球表现出更好的光催化性能。对Fe3+影响光催化活性的机理进行了讨论。     

基于聚合物中空微球构建膜内纳米空腔及其对气体渗透性能的影响

分别以四氢呋喃丙烯酸酯和双季戊四醇六丙烯酸酯为油相反应单体和交联剂,利用界面引发剂在无表面活性剂微乳液油水界面处引发聚合,制备了中空微球,浇铸形成具有纳米空腔的中空微球膜.考察了膜内纳米空腔对分离膜气体渗透性和分离性的影响.结果表明,制备的中空微球平均粒径为116. 7 nm,中空结构明显,壳层厚度为10～20 nm;中空微球膜的渗透分离性能较壳层材料的本征值有显著提升,在35℃,0. 2 MPa条件下,CO_2的渗透系数增大1. 4～5. 7倍,且分离系数也有所提升.     

Na~+,Li~+,Bi~(3+)掺杂CaWO_4∶Eu~(3+)荧光粉的制备及发光特性

采用微波辅助加热法合成了Na~+,Li~+,Bi~(3+)掺杂的CaWO_4∶Eu~(3+)荧光粉.利用X射线衍射仪和扫描电子显微镜对样品的微观结构进行了表征,利用荧光分光光度仪对样品的激发光谱、发射光谱和能级寿命进行了测试和分析.结果表明,掺杂浓度(摩尔分数)均为3.75%的Eu~(3+),Na~+,Li~+,Bi~(3+)掺杂的CaWO_4均保持了基质的四方晶相结构.Na~+,Li~+,Bi~(3+)单掺杂或共掺杂后的样品比CaWO_4∶Eu~(3+)样品颗粒度分别有不同程度的增加.在393 nm光激发下,掺杂Eu~(3+),Na~+及掺杂Eu~(3+),Li~+样品的发光强度比CaWO_4∶Eu~(3+)的发光强度分别提高了1.8倍和1.2倍,共掺杂Eu~(3+),Li~+,Na~+及Eu~(3+),Li~+,Bi~(3+)的样品发光均有所减弱.在254和393 nm光激发下,掺杂Li~+的CaWO_4∶Eu~(3+)样品的荧光寿命最短.同一样品在393 nm光激发下的荧光寿命短于254nm光激发下的荧光寿命.     

磁性SiO2/PSt中空复合微球的细乳液法制备及表征

采用双原位细乳液聚合工艺,将疏水改性的磁性纳米粒子(MNP)加入到细乳液反应体系的油相中,利用增长的聚合物和单体TEOS之间的相分离原理,实现了聚合物的生成和TEOS的水解缩合同步进行,一步获得了磁性SiO2/PSt中空复合微球.通过红外光谱(FTIR)、透射电镜(TEM)、热重差热分析(TGA/DSC)和振动磁强计(VSM)对中空复合微球进行了表征.结果表明,制备的SiO2/PSt中空复合微球的尺寸范围为300～600 nm,当加入磁性纳米粒子后,得到的磁性SiO2/PSt中空微球保持了原来的中空结构,中空复合微球内腔的大小可以通过改变单体TEOS的加入量来控制.SiO2/PSt中空微球对磁性纳米粒子的包封率达到了86%.磁性SiO2/PSt中空复合微球具有超顺磁性,饱和磁强度值为14.7 emu/g.     

基于3D受限自组装构筑中空介孔氧化硅/碳复合微球

发展简单、高效、可控的方法来制备中空介孔微球是介孔材料领域的研究热点.本工作结合嵌段共聚物的三维受限自组装(3D-CSA)和自模板碳化策略,建立了一种构筑中空介孔微球的新方法 .首先,采用乳液-溶剂挥发法实现嵌段共聚物与全氟辛烷(PFO)在3D受限空间的分级组装,获得了核-壳结构微球,其中壳层由微相分离的嵌段共聚物构成.然后,在壳层的连续相选择性地复合氧化硅,既实现了无机框架的负载,又实现了对连续相聚合物链选择性交联.对复合微球进行煅烧处理后,实现了壳层连续相聚合物的选择性碳化,获得了中空介孔氧化硅/碳复合微球.本研究系统地阐述了核-壳型分级结构微球的形成机理和必备条件,研究了氧化硅前驱体添加量和嵌段共聚物分子量对中空介孔氧化硅/碳复合微球形貌的影响,为制备中空介孔微球材料提供了一种简便、可控的方法.     

Preparation and up-conversion luminescence of hollow La2O3:Ln (Ln = Yb/Er, Yb/Ho) microspheres

Hollow La(2)O(3):Ln (Ln = Yb/Er, Yb/Ho) microspheres with up-conversion (UC) luminescence properties were successfully synthesized via a facile sacrificial template method by employing carbon spheres as hard templates followed by a subsequent heating process. The structure, morphology, formation process, and fluorescent properties are well investigated by various techniques. The results indicate that the hollow La(2)O(3):Ln microspheres can be well indexed to the hexagonal La(2)O(3) phase. The hollow La(2)O(3):Ln microspheres with uniform diameter of about 270 nm maintain the spherical morphology and good dispersion of the carbon spheres template. The shell of the hollow microspheres consists of numerous nanocrystals with the thickness of approximately 40 nm. Moreover, the possible formation mechanism of evolution from the carbon spheres to the amorphous precursor and to the final hollow La(2)O(3):Ln microspheres has also been proposed. The Yb/Er and Yb/Ho codoped La(2)O(3) hollow spheres exhibit bright up-conversion luminescence with different colors derived from different activators under the 980 nm NIR laser excitation. Furthermore, the doping concentration of the Yb(3+) is optimized under fixed concentration of Er(3+)/Ho(3+). This material may find potential applications in drug delivery, hydrogen and Li ion storage, and luminescent displays based on the uniform hollow structure, dimension, and UC luminescence properties.     

Shell-in-Shell TiO2 hollow microspheres and optimized application in light-trapping perovskite solar cells

The shell-in-shell structured TiO₂ hollow microspheres with enhanced light scattering ability were synthesized via a facile one step hydrothermal process. The diameter of the microsphere is about 1.5 μm, the core of the unique shell-in-shell structure is composed of TiO₂ nanoparticles with a diameter of about 15 nm, while the shell is constructed with ∼50 nm TiO₂ nanocubes. The hollow space between the outer shell and the inner shell is about 230 nm. The formation mechanism of the unique shell-in-shell structure is interpreted. The design and the optimized application of shell-in-shell structured TiO₂ hollow microspheres in the light-trapping perovskite solar cells are also investigated. Owing to the light scattering properties of the shell-in-shell structure of the hollow microsphere, the optimized photoelectrode exhibits an enhanced photoelectric conversion efficiency of 4.29% using perovskite CH₃NH₃PbI₃ as the sensitizer. The shell-in-shell hollow TiO₂ microsphere shows a 21.2% increase in conversion efficiency when compared with P₂₅ nanoparticels photoanode. The conversion efficiency enhancement is mainly attributed to the increase of short-current density induced by the light scattering effect.     

LaAlO3 hollow spheres: synthesis and luminescence properties

Nearly monodisperse LaAlO(3) hollow spheres are synthesized by a novel precursor thermal decomposition method. Spherical colloids of capsulelike precursors with uniform diameters of 273 ± 35 nm have been synthesized by a solvothermal method. These spherical colloids could convert to LaAlO(3) hollow spheres with diameters of 166 ± 26 nm by a thermal decomposition process. The thermal transformation process from the precursors to LaAlO(3) was characterized by thermogravimetric analysis (TGA), X-ray diffraction (XRD), and the Fourier transform infrared spectroscopy (FT-IR). By the doping of various lanthanide ions (Sm(3+), Eu(3+), and Tb(3+)), the emission luminescence of lanthanide-doped LaAlO(3) hollow microspheres can be tuned from red to green. In particular, these luminescent LaAlO(3) hollow spheres can be well dispersed in polar solvents such as the ethanol and water, which broadens the range of potential applications of these hollow spheres. The UV-vis absorption spectra show energy absorption at 211, 223, and 313 nm corresponding to the host lattice absorption and charge-transfer transitions. The results are in good agreement with the peaks observed in the excitation spectra.     

Time-dependent control of hole-opening degree of porous ZnO hollow microspheres

Well-designed, monodispersed porous ZnO hollow microspheres with controlled hole-opening were successfully synthesized by a facile two-step solution route at low temperature. The hollow microspheres having average diameter of 3-4 μm showed time-dependent hole-opening, i.e. 4-100% for 15-75 min. The hole-opening percentage increases linearly with time until complete opening. The ZnO hollow microspheres also exhibited a high surface area (34 m(2) g(-1)), a large pore volume (0.19 cm(3) g(-1)) and an average pore diameter of 3.8 nm. A plausible growth mechanism for the formation of ZnO hollow microspheres was also proposed.     

Room temperature synthesis of hollow CdMoO(4) microspheres by a surfactant-free aqueous solution route

Hollow cadmium molybdate microspheres have been successfully prepared via a template-free aqueous solution method with the assistance of NaCl at room temperature. The structure and morphology of the CdMoO(4) hollow microspheres were characterized by X-ray diffraction, field-emission scanning electron microscopy, and transmission electron microscopy. The microspheres have diameters of 3-6 microm and hollow interiors of 2-3 microm. The shell is composed of numerous single-crystalline nanorods with diameters of 30-120 nm and lengths of 1-2 microm which are radially oriented to the center. A certain concentration of NaCl plays a key important role in the formation process of hollow microspheres, which might provide a suitable chemical environment to favor the formation of hollow CdMoO(4) microspheres. A possible NaCl-induced Ostwald ripening process is proposed for the formation of hollow CdMoO(4) microspheres on the basis of scanning electron microscopy observation of intermediate products at different precipitation stages.     

简单方法制备羟基磷灰石中空微球

无需添加任何有机物和金属离子, 以易得的中空球形碳酸钙(CaCO3)与磷酸氢二钠(Na2HPO4)作为反应物在常压下制备出羟基磷灰石中空微球. 通过场发射扫描电子显微镜(FESEM)、扫描电子显微镜(SEM), X射线粉末衍射(XRD)等手段对制备的羟基磷灰石中空微球的结构、组成和形貌进行了表征, 考察了不同反应温度对中空球形貌的影响. 实验结果表明, 所制备的羟基磷灰石微球是由短针状的纳米粒子组成的, 直径为2-4 μm. 对反应机理进行了初步探讨.     

锌离子掺杂的二氧化钛介孔空心微球的制备及光催化性能

以二氧化硅为模板,钛酸四丁酯(TBOT)为钛源,硝酸锌为锌源,采用溶胶凝胶法制备了锌离子掺杂的介孔二氧化钛空心微球。采用X射线衍射(XRD)、比表面积(BET)、透射电镜(TEM)、扫描电镜(SEM)和X射线光电子能谱(XPS)等技术对样品进行表征,以亚甲基蓝(MB)的光催化降解为目标反应评价其光催化活性。结果表明,去核之后的复合微球为空心微球,壁厚为20 nm左右。钛酸四丁酯溶液的滴加时间对微球的形貌影响较大,当滴加时间大于15 min时,可以得到结构清晰的空心微球。用氢氧化钠溶液去除二氧化硅核,反应90 min,二氧化硅可以被完全去除。X射线衍射表明,实验得到的掺杂锌离子的空心微球和没有掺杂锌离子的空心微球都是锐钛矿。当锌离子的摩尔分数为0.3%时,二氧化钛空心微球的晶粒尺寸最小,比表面积最大,催化亚甲基蓝降解的效率最高。     

锌离子掺杂的二氧化钛介孔空心微球的制备及光催化性能

以二氧化硅为模板,钛酸四丁酯（TBOT）为钛源,硝酸锌为锌源,采用溶胶凝胶法制备了锌离子掺杂的介孔二氧化钛空心微球。采用X射线衍射（XRD）、比表面积（BET）、透射电镜（TEM）、扫描电镜（SEM）和X射线光电子能谱（XPS）等技术对样品进行表征,以亚甲基蓝（MB）的光催化降解为目标反应评价其光催化活性。结果表明,去核之后的复合微球为空心微球,壁厚为20nm左右。钛酸四丁酯溶液的滴加时间对微球的形貌影响较大,当滴加时间大于15min时,可以得到结构清晰的空心微球。用氢氧化钠溶液去除二氧化硅核,反应90min,二氧化硅可以被完全去除。X射线衍射表明,实验得到的掺杂锌离子的空心微球和没有掺杂锌离子的空心微球都是锐钛矿。当锌离子的摩尔分数为0.3%时,二氧化钛空心微球的晶粒尺寸最小,比表面积最大,催化亚甲基蓝降解的效率最高。     

空心玻璃微珠对聚氨酯泡沫燃烧和力学性能的影响

通过向聚氨酯发泡体系中添加空心玻璃微珠,制备出空心玻璃微珠聚氨酯三相泡沫.研究了空心玻璃微珠添加量、聚磷酸铵(APP)用量、膨胀阻燃体系(IFR)浓度等因素对聚氨酯泡沫燃烧和力学性能的影响.结果表明,单独添加空心玻璃微珠对聚氨酯泡沫的氧指数和水平燃烧速度影响不大.添加APP或IFR后,空心玻璃微珠聚氨酯三相泡沫的阻燃效...