室温固相研磨制备椭球形活性碳酸钙

以Span60为添加剂,利用Ca(Ac)2.H2O与Na2CO3在室温下进行固相研磨反应合成椭球形活性碳酸钙,考察了Span60用量对样品活性、分散性的影响。用X射线衍射仪(XRD)分析、扫描电子显微镜(SEM)、傅立叶变换红外吸收光谱(FTIR)、粒度分析等手段对所得样品进行了表征,探讨了椭球形碳酸钙的形成机理。结果表明,Span60对碳酸钙粒子的结构和形貌具有调控作用,微米级椭球形碳酸钙是由纳米级小颗粒组装而成。在Span60的用量4%的条件下,可制得活性高、分散性好、粒度为1~3μm的椭球形碳酸钙。     

超细YF_3与GdF_3纳米晶的合成及其上转换发光

当使用液固溶法(LSS法)制备分散性纳米晶时,将传统油酸/油酸钠/酒精反应体系中的NaOH用氨水取代时,氨水将会与油酸形成新的表面活性剂油酸铵,这样就可以合成各种超细分散性的REF3纳米晶(RE代表稀土元素)。在这种新的反应体系中,合成了平均直径小于10 nm的YF3和GdF3超细颗粒,X射线与透射电镜测试表明YF3是正交相,而GdF3是面心立方结构,空间群为Fm3m,晶格常数为0.582 9 nm。在980 nm半导体激光器激发下,可检测到YF3∶Yb/Er在515~570 nm处有较强的绿色发光峰、645~675 nm处有较强的红色发光峰,呈橙色发光。YF3∶Yb/Tm和GdF3∶Yb/Tm样品在460~490 nm处有较强的蓝色发光峰,而在800 nm附近有更强的近红外发光峰。由于其超细的尺寸及红外上转换发光特性,合成的样品在生物成像、生物标签等方面有潜在的应用价值。     

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.     

稀土纳米复合氧化物RE_2O_3∶Eu(RE=Y,Gd)的制备及特性

以甘氨酸辅助的燃烧法和非晶态稀土DTPA配合物前驱体热分解法制备了Y2 O3 ∶Eu和Gd2 O3 ∶Eu纳米材料。X射线衍射表明燃烧法和配合物前驱体热分解法制备的纳米Y2 O3 ∶Eu均为立方相 ,而Gd2 O3 ∶Eu纳米材料则随制备条件不同可得到立方相或单斜相两种产物 ,发射光谱证实了这一结论。通过透射电子显微镜、扫描电子显微镜对不同方法制备的纳米材料的尺寸、形貌也进行了表征     

多种形貌YF_3:Eu~(3+)纳米发光材料的水热合成与性能比较

在不同表面活性剂辅助的水热条件下合成出纺锤形、花束状、纳米束和削角八面体形的YF3:Eu3+纳米发光材料,对其结构和性能进行了表征.XRD分析表明:样品为结晶良好的正交相YF3.由FESEM与TEM照片可见,不同表面活性剂的条件下,所合成样品的形貌不同.SEAD显示所得样品分别为多晶和单晶结构,EDX显示所得样品中含有F,Y和Eu三种元素.荧光光谱表明:YF3:Eu3+纳米晶的最强发射峰位于591nm,对应Eu3+的5D0→7F1的磁偶极跃迁发射,说明Eu3+占据YF3基质中Y3+晶格点的C2对称格位上.不同形貌样品的荧光光谱强度不同.     

YF3包覆Li(Li0.22Ni0.17Mn0.61)O2正极材料的性能

富锂层状氧化物作为锂离子电池正极材料具有高比容量优势.采用草酸盐共沉淀法制备Li(Li0.22Ni0.17Mn0.61)O2,并用YF3包覆电极.采用X射线衍射(XRD)、扫描电子显微镜(SEM)和X射线能谱分析(EDS)表征材料结构、观察材料形貌.结果表明,材料颗粒尺寸在100～200 nm范围,YF3包覆不会改变材料结构和形貌.电化学恒流充放电测试表明,YF3包覆Li(Li0.22Ni0.17Mn0.61)O2电极的比容量,尤其倍率比容量明显提高.60 mA·g-1电流密度下包覆电极材料30周循环后其比容量保持在220 mAh·g-1以上,1500 mA·g-1电流密度下其比容量仍可达150 mAh·g-1.电化学阻抗谱(EIS)测试结果表明,YF3包覆电极电荷转移电阻和扩散阻抗均明显降低,有利于电化学性能改善.     

稀土纳米复合氧化物RE2O3：Eu（RE=Y，Gd）的制备及特性

以甘氨酸辅助的燃烧法和非晶态稀土DTPA配合物前驱体热分解法制备了Y2O3:Eu和Gd2O3:Eu纳米材料。X射线衍射表明燃烧法和配合物前驱体热分解法制备的纳米Y2O3：Eu均为立方相,而GdO3:Eu纳米材料则随制备条件不同可得到立方相或单斜相两种产物,发射光谱证实了这一结论。通过透射电子显微镜、扫描电子显微镜对不同方法制备的纳米材料的尺寸、形貌也进行了表征。     

桑葚状CaF_2纳米材料的合成及CaF_2:Yb~(3+)的光学性质

通过一步水热法合成了分散性良好、尺寸均一的桑葚状CaF2纳米材料.采用X射线粉末衍射(XRD)、场发射扫描电子显微镜(FESEM)和透射电子显微镜(TEM)对产物的结构、形貌及尺寸进行了表征,发现CaF2纳米材料是由尺寸约为50 nm的纳米粒子构成.通过对不同反应阶段产物的分析提出了其形成机理.研究了Yb3+掺杂CaF2纳米材料的近红外发光性质.     

LaF3纳米片和棒束的选择性合成及表征

室温条件下,以简单的液相法,通过改变氟源NaBF4和K2SiF6,制得不同形貌的LaF3纳米晶(片及棒束).X射线衍射(XRD)结果显示所得的2种不同形貌的产物均为结晶良好的六方相LaF3.场发射扫描电子显微镜(FE-SEM)、透射电子显微镜(TEM)结果表明由NaBF4制得大量均匀、厚度约为20 am的六边形纳米片....     

孔状Co_3O_4纳米片和纳米棒的选择性合成和表征(英文)

利用两步实验选择性合成孔状Co3O4纳米片和纳米棒:首先,以Co(NO3)2·6H2O,NaOH和不同量的NH4F为原料在120℃水热6h的条件下合成了Co(OH)2-Co3O4纳米片(S1)和Co(OH)F-Co3O4纳米棒(S2);然后将所得纳米片和纳米棒在400℃时加热2h即得到多孔的Co3O4纳米片和纳米棒。所得产物用X射线衍射(XRD)、场发射扫描电子显微镜(FE-SEM)和透射电子显微镜(TEM)进行了表征。此外电化学测试表明Co3O4纳米棒的电容量比Co3O4纳米片的更大。     

超细YF3与GdF3纳米晶的合成及其上转换发光

当使用液固溶法（LSS法）制备分散性纳米晶时,将传统油酸/油酸钠/酒精反应体系中的NaOH用氨水取代时,氨水将会与油酸形成新的表面活性剂油酸铵,这样就可以合成各种超细分散性的REF₃纳米晶（RE代表稀土元素）。在这种新的反应体系中,合成了平均直径小于10nm的YF₃和GdF₃超细颗粒,X射线与透射电镜测试表明YF₃是正交相,而GdF₃是面心立方结构,空间群为Fm3m,晶格常数为0.5829nm。在980nm半导体激光器激发下,可检测到YF₃：Yb/Er在515~570nm处有较强的绿色发光峰、645~675nm处有较强的红色发光峰,呈橙色发光。YF：Yb/Tm和GdF₃：Yb/Tm样品在460~490nm处有较强的蓝色发光峰,而在800nm附近有更强的近红外发光峰。由于其超细的尺寸及红外上转换发光特性,合成的样品在生物成像,生物标签等方面有潜在的应用价值。     

Synthesis and spectral properties of Eu-doped YF3 nanobundles

YF₃:Eu³⁺ nanobundles were synthesized by a facile microemulsion method. Analysis of X-ray diffraction, scanning electron microscope, and transmission electron microscopy reveals that each nanobundle consists of numerous nanowhiskers with a mean length of ∼500 nm and a mean diameter of ∼2 nm. Under 393-nm excitation, the luminescence was dominated by ⁵D₀ → ⁷F₁ transition, indicating the inversion symmetry of Eu³⁺ site. The luminescence intensity increased with increasing Eu³⁺ concentration, up to about 30 mol%, and then decreased abruptly. The peak positions and spectral shapes of emissions were independent of Eu³⁺ concentration. Finally, the critical distance of energy transfer was calculated.     

Structural relationships and mechanisms for the stoichiometry change from MX3 (YF3-type) through MX2 (fluorite-type) to M2X3 (C-type sesquioxide)

Structures produced by inducing stoichiometry changes in crystalline fluorides and oxide-fluorides of yttrium by pyrohydrolysis have been studied by X-ray powder diffraction and electron microscopy. The structures of YF₃, various fluorite-related intermediates and the ultimate product of hydrolysis, Y₂O₃, are all closely related. The pyrohydrolysis is topotactic; the anion sublattice remains intact and vacancies and oxygen substitute for fluorine on the anion sublattice in an ordered, cooperative way to produce fully ordered product structures. A ‘unit slip’ mechanism, involving the most favourable slip systems for a primitive cubic sublattice, 〈001〉{110} and 〈001〉{110}, is postulated as a possible mechanism for the process.     

Über fluorit- und tysonitverwandte Ordnungsphasen im System CaF2YF3

A systematic phase study has been made on the CaF₂YF₃ system with particular emphasis on the attainment of equilibrium at low temperatures. Long annealing has produced three ordered phases: Ca₂YF₇ (t), Ca₉Y₅E₃₃ (rhα), and Ca_8?δY_5+δF_31+δ = Ca_7+δY_6?δF_32?δ (rhβ). These phases crystallize as anion-excess fluorite-related superstructures and can be described as members of the homologous series (Ca, Y)_mF_2m+5 with m = 15, 14, and 13. In the fluorine-rich region of the system are found two high-temperature phases: a solid solution with tysonite structure (Z = 2) and a related, monoclinic, ordered phase with the formula Ca₃Y₇F₂₇.     

Synthesis and upconversion luminescence properties of YF3:Yb/Tm octahedral nanocrystals

YF₃:Yb³⁺(20%)/Tm³⁺(2%) octahedral nanocrystals were synthesized by a microemulsion method with NH₄HF₂. Pumped with a 980-nm diode laser, the nanocrystals emitted weak blue and intense ultraviolet light. Especially, unusual ³P₂ → ³H₆ (∼265 nm) and ³P₂ → ³F₄ (∼309 nm) emissions, coming from a five-photon excitation process, were observed. The emissions from ¹D₂ and ¹I₆ were much stronger than those from ¹G₄ and ³H₄. The upconversion mechanism was discussed in detail.     

Enhanced ultraviolet up-conversion emissions of Tm/Yb codoped YF3 nanocrystals

Tm³⁺/Yb³⁺ codoped rod-like YF₃ nanocrystals were synthesized through a facile hydrothermal method. After annealing in an argon atmosphere, the nanocrystals emitted bright blue and intense ultraviolet (UV) light under a 980-nm continuous wave diode laser excitation. Up-conversion emissions centered at ∼291 nm (¹I₆ → ³H₆), ∼347 nm (¹I₆ → ³F₄), ∼362 nm (¹D₂ → ³H₆), ∼452 nm (¹D₂ → ³F₄), ∼476 nm (¹G₄ → ³H₆), ∼642 nm (¹G₄ → ³F₄), and ∼805 nm (³H₄ → ³H₆) were recorded using a fluorescence spectrophotometer. Especially, enhanced UV emissions were studied by changing Yb³⁺/Tm³⁺ doping concentrations, the annealing temperatures, and the excitation power densities. A possible mechanism, energy transfer-cross relaxation-energy transfer (ET-CR-ET), was proposed based on a simple rate-equation model to elucidate the process of the enhanced UV emissions.     

Size-dependent upconversion luminescence in YF3:Yb/Tm nanobundles

The upconversion luminescent properties of YF₃:Yb³⁺(20%)/Tm³⁺(1%) nanobundles with different sizes (240-500 nm in length) were studied under 980-nm excitation. Ultraviolet (¹I₆ → ³F₄/³H₆ and ¹D₂ → ³H₆), blue (¹D₂ → ³F₄ and ¹G₄ → ³H₆), red (¹D₂ → ³H₄, ¹G₄ → ³F₄, and ³F₃ → ³H₆), and near infrared (³H₄ → ³H₆) emissions were observed. The results indicated that the relative intensity of the ultraviolet to the blue as well as the blue to the near infrared increased with decreasing the size of nanobundles. Especially, the position of the dominant red emission peak varied with the size of nanobundles. As the length of nanobundles increased to 500 nm, unusual ³F₃ → ³H₆ transition was observed, which was theoretically explained considering the decrease of the nonradiative transition rate of ³F₃ → ³H₄.     

溶胶凝胶法合成Li3V6O16及其电化学性能研究

本文以双氧水为配位剂,以CH3COOLi·2H2O和V2O5为原料,采用溶胶凝胶法合成了一种新型的晶体Li3V6O16。随后分别采用X射线衍射(XRD)、扫描电子显微镜(SEM)、透射电子显微镜(TEM)和电子衍射(SAED)、X光电子能谱(XPS)和充放电测试等手段对材料进行了表征。SEM观察表明,产物主要是表面比较光滑的纳米片状晶体,TEM和SAED研究都证实了XRD和SEM的研究结果。充放电测试结果表明,该物质具有较高的比容量、良好的可逆性和循环稳定性。     

Influence of surfactants on the morphologies of CaCO3 by carbonation route with compressed CO2

Three surfactants, sodium dodecyl sulfate (SDS), cetyltrimethylammonium bromide (CTAB) and polyoxyethylene-80-sorbitan monooleate (Tween 80), were used to control the growth of CaCO₃ crystals by carbonation route using Ca(OH)₂ and compressed CO₂. The obtained CaCO₃ particles were characterized by scanning electron microscopy (SEM) and X-ray diffraction (XRD) techniques. The effects of surfactants on the morphology of the particles were studied. It was demonstrated that Tween 80 and SDS have obvious effect on the morphology of CaCO₃ particles, while CTAB does not affect morphology considerably. The possible mechanism has been discussed on the basis of the binding of the surfactants to the certain face of the crystals.