EuF3 纳米晶/PNIPAm复合水凝胶的制备及荧光温敏性能

以十一烯酸为表面活性剂, 采用液体-固体-溶液法(LSS)制备了EuF3纳米晶; 将其用CCl4处理, 得到表面修饰有C-Cl基团的功能化EuF3纳米晶; 通过原子转移自由基聚合(ATRP)制备EuF3 /聚N-异丙基丙烯酰胺(EuF3/PNIPAm)复合温敏水凝胶. 采用HRTEM, XRD, FTIR, DSC及PL等对EuF3 纳米晶及EuF3/ PNIPAm 复合凝胶的微观结构与性能进行了表征, 用变温荧光光谱研究了环境温度对复合凝胶荧光性能的影响. 结果表明, EuF3纳米晶呈六方相晶型; 粒径呈多分散分布, 且相对集中于10, 20和50 nm. 该复合凝胶的较低临界溶解温度(LCST)随纳米晶含量的增加而下降, 环境温度与纳米晶含量对复合凝胶的荧光特性产生明显影响.     

单分散CdS纳米晶/PNIPAM复合水凝胶的制备及其温敏荧光特性

采用液体-固体-溶液法(LSS)制备单分散CdS纳米晶;通过自由基聚合制备单分散CdS纳米晶/聚N-异丙基丙烯酰胺(CdS/PNIPAM)复合温敏水凝胶.采用HRTEM、XRD、FTIR、DSC、PL等对CdS纳米晶、CdS/PNIPAM温敏复合凝胶的微观结构与性能进行了表征,变温荧光光谱研究了温度对凝胶荧光性能的影响.结果表明,CdS纳米晶粒径约为2.8 nm,单分散性良好;复合凝胶的荧光发射强度与环境温度存在一定的关联性,且呈可逆性.     

PNIPAm温敏纳米纤维膜：交联作用下的形貌稳定性和响应行为

聚N-异丙基丙烯酰胺(PNIPAm)交联温敏纳米纤维膜作为一种相变温度易于控制的新兴响应性材料,克服了传统PNIPAm块状水凝胶的生产成本高、响应速率慢和PNIPAm非交联温敏纳米纤维耐水性差的缺点,受到广泛研究并应用于智能开关、温度致动器、水油分离、药物、细胞控制释放和伤口敷料等领域。形貌稳定性和快速响应性是温敏纳米纤维膜在重复体积变化过程中最大的挑战,同时也作为评价PNIPAm温敏纳米纤维膜的实用性最重要指标引起了人们广泛的关注。本文全面综述了PNIPAm温敏纳米纤维膜近二十年来国内外的突破性进展和非交联作用下PNIPAm温敏纳米纤维膜的形貌变化和响应性,重点综合分析了物理和化学交联中交联反应类型、交联度、交联时间和交联分子量对PNIPAm温敏纳米纤维膜的形貌稳定性和响应行为的影响,为之后纤维膜的交联处理提供了理论支持,并对PNIPAm温敏纳米纤维膜的发展及应用前景进行了展望。     

一锅法制备YF_3:Yb~(3+)-Er~(3+)纳米晶复合PNIPAm-co-PAA纳凝胶及其荧光温敏行为

采用巯基乙胺为配体,以硝酸铒(Er(NO3)3),硝酸镱(Yb(NO3)3),硝酸钇(Y(NO3)3)和氟化铵(NH4F)为原料,水热法制备表面含NH2基团的活性YF3:Yb3+-Er3+纳米晶;以过硫酸钾(K2S2O8)为引发剂,借助1-乙基-(3-二甲基氨基丙基)碳酰二亚胺(EDC)与N-羟基丁二酰亚胺(NHS)的偶联反应,在活性纳米晶存在下,进行N-异丙基丙烯酰胺(NIPAm),N,N'-亚甲基双丙烯酰胺(BIS)与丙烯酸的自由基共聚合,一锅法制备了YF3:Yb3+-Er3+/PNIPAm-co-PAA荧光温敏纳凝胶.对制备的纳米晶及纳凝胶的结构与荧光性能进行了表征.结果表明,纳米晶的粒径为6~10 nm,呈单分散分布;纳凝胶的粒径呈多分散分布,粒径主要分布在100~300 nm.PL光谱分析表明,活性YF3:Yb3+-Er3+纳米晶的4F7/2→4I15/2跃迁,在483和496 nm处产生明显的能级劈裂;纳凝胶中,该能级劈裂依然存在,但随温度升高发生耦合;环境温度对纳凝胶的上转换发光强度产生明显影响.     

温敏性聚(N-异丙基丙烯酰胺)/聚氨酯-β-环糊精互穿网络水凝胶的溶胀特性

利用互穿网络（IPN）技术，以温敏性聚（N－异丙基丙烯酰胺）（PNIPAm)、聚氨酯（PUE）以及具有分子包合效应的β－环糊精（β－CD）为原料，采用分步法和同步法制备了新型互穿网络水凝胶。通过对水凝胶溶胀行为的考察，可知水凝胶具有同PNIPAm相似的在低临界溶解温度（LCST）处的相转变行为，且PUE／PNIPAm的组成比，线型PNIPAm分子量以及交联剂用量等因素对IPN水凝胶的溶胀特性与温敏特性有显著的影响。     

聚N-异丙基丙烯酰胺/纳米SiO2复合水凝胶的合成及溶胀性能

通过纳米SiO2的表面功能化,在其表面引入乙烯基功能基团,在H2O／THF的混合溶剂中,超声分散后,交联剂N,N′-亚甲基双丙烯酰胺存在时,于25℃下使其与N-异丙基丙烯酰胺共聚,制得聚N-异丙基丙烯酰胺,纳米SiO2复合水凝胶,并用FT-IR和SEM对产物进行了表征,研究了凝胶的溶胀动力学,消溶胀动力学和温度敏感性,实验结果表明,纳米SiO2的引入,改善了聚N-异丙基丙烯酰胺水凝胶在低温时的溶胀性能和在高温时对水的释放性能,并讨论了引起这些性能改变的原因。     

腐植酸钠/聚N-异丙基丙烯酰胺/粘土杂化水凝胶的合成及脱色性能

以N-异丙基丙烯酰胺单体、粘土和腐植酸钠为原料合成了温敏腐植酸钠/聚N-异丙基丙烯酰胺/粘土（SH/PNIPA/clay）系列水凝胶。用红外光谱分析仪对其内部相互作用进行了研究,并用紫外可见分光光度计对水凝胶吸附-解吸亚甲基蓝的性能进行了测试。实验结果表明凝胶中SH与PNIPA形成了氢键;凝胶对亚甲基蓝（MB）的吸附和解吸能力受腐植酸钠的含量、粘土含量、亚甲基蓝的起始浓度和温度的影响。２％粘土含量和低温条件有利于凝胶吸附和解吸。     

上转换荧光响应性复合纳米凝胶的制备及荧光能量传递行为

采用水热法合成NaYF₄∶Yb³⁺,Er³⁺稀土纳米晶, 再经3-苄基三硫代碳酸酯基丙酸(BSPA)修饰, 制得功能化纳米晶体; 以罗丹明6G(R6G)为母体荧光染料, 经一系列反应合成了乙烯基功能化单体罗丹明6G酰基邻羧基苯甲肼腙(R6GHA); 将功能化纳米晶体与R6GHA构成荧光共振能量传递(FRET)的“给体/受体”对, 通过可逆加成断裂链转移(RAFT)聚合和“点击化学”反应, 合成具有多重响应性复合荧光纳米凝胶NaYF₄∶Yb³⁺,Er³⁺/PNIPAm-co-R6GHA. 采用TEM, XRD, FTIR和DSC对产物的微观结构进行了表征; 采用上转换荧光光谱(PL)研究了该复合纳米凝胶对pH值、 环境温度和不同金属离子的荧光响应行为, 并对相关机理进行了探讨. 结果表明, 环境温度变化对复合纳米凝胶的荧光发射具有显著影响, 且该复合纳米凝胶对Hg²⁺具有选择性荧光响应; 在H⁺或Hg²⁺作用下, 复合纳米凝胶中纳米晶和R6GHA之间会发生荧光共振能量传递; 通过纳米凝胶中纳米晶与R6GHA特征荧光发射峰比率的变化, 实现对Hg²⁺的检测.     

肿瘤热疗化疗联合治疗用温敏磁性复合粒子的磁热性能

采用无皂乳液聚合法制备了Fe₃O₄/P（N-异丙基丙烯酰胺-共-丙烯酰胺）[P（NIPAAm-co-Am）]温敏磁性复合粒子,分别采用透射电镜（TEM）,振动磁强仪（VSＭ）和动态激光散射仪（DLS）对复僵粒子进行表征,并着重研究了复合粒子在交变磁场作用下的磁热性能。结果表明,Fe₃O₄纳米粒子表面包裹了一层P（NIPAAm-co-Am）温敏性聚合物,其最低临界溶解温度（LCST）约为40℃,利用磁性粒子在交变磁场下的磁热性能可使复合粒子的温度升高至LCST以上,可触发复合粒子发生体积收缩。另外,复合粒子在交变磁场下的磁热性能可通过改变磁性粒子的浓度或调节磁场来调控。     

AuNPs/PNIPAM复合颗粒的制备及其温敏性质

将金纳米颗粒(AuNPs)组装到聚N-异丙基丙烯酰胺(PNIPAM)水凝胶微球表面制备出AuNPs/PNIPAM复合颗粒. 将PNIPAM 凝胶的温敏特性与AuNPs的光学性质结合, 通过改变温度调节AuNPs的局部表面等离子共振(LSPR)吸收峰位置. 研究结果表明, 温度升高使AuNPs的LSPR吸收峰发生红移, 并且这种效应是可逆的. 同时发现, AuNPs的光学性质还可以作为表征PNIPAM水凝胶微球温敏行为的一种手段. 利用透射电镜、紫外-可见光谱仪及动态光散射仪对AuNPs/PNIPAM复合颗粒的形貌、光学性质、粒径变化等进行了分析.     

球状、立方状及空心立方状PbS纳米晶的控制合成及其形成机理

以醋酸铅为铅源,硫代乙酰胺为硫源,在表面活性剂十二烷基硫酸钠(SDS)和十六烷基三甲基溴化铵(CTAB)共同作用下,通过简单地调节水热反应的反应温度控制合成出球状、立方状和空心立方状PbS纳米晶。利用XRD、TEM对合成产物的结构和形貌进行了表征,发现合成的球状、立方状和空心立方状PbS纳米晶尺寸均一,直径为100 nm左右。对球状、立方状和空心立方状PbS纳米晶的形成机理进行了初探,结果表明反应温度较低时,水热反应初始阶段形成的PbS小颗粒呈球形,在表面活性剂SDS的烷基链模板和CTAB微胶束软模板共同作用下生成球状PbS纳米晶;反应温度较高时,水热反应初始阶段形成的PbS小颗粒由于自身的立方相岩盐晶体结构的影响有呈立方状趋势,在SDS和CTAB共同作用下产物堆积成空心立方体状或立方状。     

溶剂热法合成CdSxSe1-x棒状纳米材料

以乙二胺为溶剂，制备了直径为10～20 nm、长度100～150 nm的棒状CdS_xSe_1-x纳米晶体，并对其形成过程及机理进行了探讨。研究发现CdS_xSe_1-x纳米晶体在120 ℃下就可形成且纳米棒的形貌不受温度及反应物配比的影响。紫外-可见光谱表明得到的CdS_xSe_1-x纳米晶体的光学性质可通过简单改变反应物中S与Se的配比进行调控。     

溶剂热合成单分散硫化镉纳米晶

在双表面活性剂十八胺和油酸存在条件下, 以氯化镉和硫粉作为反应前驱物, 通过简单的溶剂热方法合成单分散性闪锌矿硫化镉纳米晶, 粒径大小在13 nm. 用X射线衍射(XRD)、透射电子显微镜(TEM)对产物的结构和形貌进行了表征, 同时对硫化镉纳米晶的紫外吸收谱和光致发光谱(PL)性能进行了表征. 实验结果表明合成的样品具有很好的发光性能, 此外溶剂热反应的温度对纳米晶的单分散性有重要影响. 并对硫化镉纳米晶的形成机理做了初步的研究.     

化学沉淀法用于多种形貌ZnS纳米晶的可控合成

以辛基酚聚氧乙烯醚(OP-10)为表面活性剂, 二甲基甲酰胺(DMF)/水为溶剂, 用沉淀法制备了纳米球、纳米棒、纳米片等多种形貌可控的ZnS纳米晶, 并且用透射电子显微镜、X射线衍射、紫外吸收、荧光光谱对其进行了表征, 并且分析了其形貌转变机理.     

金二元纳米晶超晶格的自组装和结构表征

The assembly of two-component nanocrystals (NCs) such as metals, magnets, and semiconductors into binary nanocrystal superlattices (BNSLs) provides a fabrication route to novel classes of materials. BNSLs with certain structures can exhibit the combined and collective properties of their building blocks and are widespread in the fields of electronics and magnetic devices. As most studies have focused on combined two-component NCs of different sizes for self-assembling BNSLs, there are a few studies on single-component NCs of different sizes for the construction of BNSLs; this is especially true for Au NCs. Noble metallic Au NCs are an excellent candidate material because of their exceptional chemical stability, catalytic activity, process ability, and metallic nature; these characteristics provide them unique size-dependent optical and electronic properties as well as a wide variety of applications in sensing, imaging, electronic devices, medical diagnostics, and cancer therapeutics owing to their strong interactions with external electromagnetic fields. Therefore, it is important to develop a simple and efficient procedure to build BNSLs with different sizes of Au NCs. In our study, we synthesized monodispersed (size distribution < 10%) 6.0, 7.3, and 9.6 nm Au NCs using dodecanethiol-stabilized 3.7 nm Au NCs as seeds through a seed-growth method in oleylamine. The obtained Au NCs exhibited morphology and nanocrystallinity (single-domain and polycrystalline) similar to those of Au seeds. As the size of Au NCs increased from 3.7 to 6.0, 7.3, and 9.6 nm, the surface plasmon resonance peaks narrowed and indicated a red shift. The oleylamine-functionalized 6.0, 7.3, and 9.6 nm Au NCs were mixed with 3.7 nm Au NCs at certain concentration ratios. Au BNSLs with AB₂ (hexagonal AlB₂ structure), AB₁₃ (NaZn₁₃ structure), and AB (cubic NaCl structure) type were obtained through the solvent evaporation method. The (001) plane of the AlB₂-type structure, (001) plane of the NaZn₁₃-type structure, and (100) plane of NaCl-type structure superlattices were observed through transmission electron microscopy (TEM). The effective particle size ratios (γ= D_small/D_large) serve as the critical determining factor in the formation of the BNSLs. The effective particle size of NCs is equal to the sum of the metal core diameter and twice the thicknesses of the surface ligand. In our study, the effective particle size D_small (Au seed) is 5.7 nm; the effective particle sizes D_large (6.0, 7.3, and 9.6 nm Au NCs) are 9.0, 10.3, and 12.6 nm, respectively. The effective particle size ratios γ were therefore calculated to be 0.63, 0.55, and 0.45, respectively. The relevant space filling principle predicted the stability of the AlB₂, NaZn₁₃, and NaCl-type structures in the range of 0.482 < γ < 0.624, 0.54 < γ < 0.625, and γ < 0.458, respectively; the experimental results adequately matched the relevant space filling principle. The investigation of such a single nanocomponent as a building block is noteworthy with regard to the structures and properties of BNSLs as well as the potential development of novel meta-materials.     

Preparation of nanocrystalline Na2ZrO3 for high-temperature CO2 acceptors: chemistry and mechanism

Nanocrystalline Na₂ZrO₃ was demonstrated as a promising acceptor for CO₂ capture at elevated temperatures. The mechanism of nanocrystalline Na₂ZrO₃ formation from the soft-chemistry route is elucidated by varying precursors, preparation methods, and calciantion temperatures, combining detailed characterizations by X-ray diffraction (XRD) and scanning electron microscope (SEM) at different steps in the process. The results revealed that the drying method such as spraying drying and simple evaporation-drying did not influence the final product properties. However both Na and Zr precursors had remarkable influences on the Na₂ZrO₃ formation. The solid reaction of Na intermediate and nanocrystalline ZrO₂ in the calcination was identified as the key step for the Na₂ZrO₃ formation, where the formation of molten phase Na intermediate was found to be crucial to facilitate the solid reaction. We provided principles for rational design of the chemistry for the Na₂ZrO₃ formation where the formation of Na intermediate with low melting points is essential. Pure nanocrystalline Na₂ZrO₃ can be synthesized from a mixture containing sodium nitrate and zirconoxy citrate via the formation of NaNO₃ with low melting point. However, it is not possible to form pure nanocrystalline Na₂ZrO₃ at relatively low temperatures from the mixtures of NaAc/ZrO(NO₃)₂ or NaCA/ZrOCl₂ due to the formation of Na₂CO₃ and NaCl with high melting points.     

微波溶剂热法合成纳米晶Cu2SnSe4及其结构研究

The nanocrystal Cu₂SnSe₄ was synthesized by the microwave solvothermal technique and characterized by X-ray powder diffraction (XRD), transmission electron microscope (TEM) and X-ray photoelectron spectroscopy (XPS). Results show that the technique is fast, simple and energy saving, and the average size of the product is 20～30 nm. Optical absorption spectrum of Cu₂SnSe₄ shows that product with a band gap of 2.36 eV is a better semiconductor.     

碲化镉纳米晶与聚合物复合研究进展

综述了近年来半导体纳米晶CdTe/聚合物复合材料在电致发光器件和复合发光材料方面的研究和应用进展情况,详细介绍了CdTe与水溶性高分子,非水溶性高分子以及生物大分子的复合情况,并展望了其发展前景。     

聚合物-二氧化硅复合基材中CdS纳米晶的合成

本文报道在Sol-gel基材中制备由聚合物稳定的CdS纳米晶的新方法， 即通过甲基丙烯酸镉与甲基丙烯酸羟乙酯共聚合合成了含有Cd 2+的聚合物微凝胶, 在聚合物微凝胶网络中原位聚合正硅酸乙酯形成聚合物互穿的Sol-gel复合基材. 再向该聚合物/二氧化硅复合基材中通入H2S气体得到CdS纳米晶. 在聚合物网络中原位聚合正硅酸乙酯可以降低纯二氧化硅材料的脆性; 另一方面, 二氧化硅可以作为增强剂增加聚合物材料的强度. 因此, 在我们合成的聚合物/二氧化硅复合基材中制备的CdS纳米晶将具有很好的应用前景.