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1.
通过溶液浇筑法制备了核-壳结构的硅烷偶联剂3-氨丙基三乙氧基硅烷(3-APTS)交联的SrTiO3/PVDF复合物薄膜,对其进行了XRD、FTIR、TG、DSC、SEM、介电和铁电性能测试。研究发现,使用硅烷偶联剂有助于SrTiO3在复合物薄膜中实现均匀分散,其可能与硅烷偶联剂可以被用作交联剂连接聚合物和无机材料形成核-壳结构有关。SrTiO3(ST)的引入有助于提高复合物薄膜的结晶性,但是会导致电活性β-晶相含量的轻微减少。当ST的质量含量达到30%时,复合物薄膜的介电常数可以增大至纯PVDF的2.5倍,并且不会引起介电损耗的明显增加;同时,该复合物薄膜的剩余极化率(Ps)也可以增大到原来的2倍左右。我们的研究表明,在PVDF中引入硅烷偶联剂表面改性的ST是制备具有良好分散性的复合物薄膜以及提升其铁电和介电性能的一种有效方法。  相似文献   

2.
通过溶液浇筑法制备了核-壳结构的硅烷偶联剂3-氨丙基三乙氧基硅烷(3-APTS)交联的SrTiO_3/PVDF复合物薄膜,对其进行了XRD、FTIR、TG、DSC、SEM、介电和铁电性能测试。研究发现,使用硅烷偶联剂有助于SrTiO_3在复合物薄膜中实现均匀分散,其可能与硅烷偶联剂可以被用作交联剂连接聚合物和无机材料形成核-壳结构有关。SrTiO_3(ST)的引入有助于提高复合物薄膜的结晶性,但是会导致电活性β-晶相含量的轻微减少。当ST的质量含量达到30%时,复合物薄膜的介电常数可以增大至纯PVDF的2.5倍,并且不会引起介电损耗的明显增加;同时,该复合物薄膜的剩余极化率(Ps)也可以增大到原来的2倍左右。我们的研究表明,在PVDF中引入硅烷偶联剂表面改性的ST是制备具有良好分散性的复合物薄膜以及提升其铁电和介电性能的一种有效方法。  相似文献   

3.
FexOy/SBA-15介孔分子筛的合成以及性能研究   总被引:1,自引:0,他引:1       下载免费PDF全文
在酸性溶液中利用溶胶凝胶-pH值控制两步法直接合成FexOy/SBA-15介孔分子筛,同时利用场发射扫描电子显微镜(FESEM)、小角度X射线衍射(Low-angle XRD)、透射电子显微镜(TEM)以及振动样品磁强计(VSM)对制备的各种SBA-15介孔分子筛进行结构以及性能的测试、表征。结果显示FexOy均匀地分散在SBA-15的骨架中,而且会对SBA-15介孔分子筛起钉轧作用。而后着重研究了FexOy的加入对SBA-15介孔分子筛的热稳定性、催化特性以及磁学性能的影响。FexOy的引入可以增加制备的SBA-15介孔分子筛的热稳定性;FexOy的引入可以改善SBA-15介孔分子筛的催化活性,得到了开口的、石墨化程度较好的纳米碳管。FexOy的引入使SBA-15介孔分子筛具有明显的铁磁性。  相似文献   

4.
采用水热法合成出具有不同V、P物质的量之比的BiVO4/BiPO4复合物.nV/nP分别为:0.1/9.9、0.5/9.5、1/9、3/7、5/5.采用 XRD、FE-SEM、EDS、拉曼、可见光光度计、漫反射以及电化学等测试手段对BiVO4/BiPO4复合物进行表征.在可见光条件下降解亚甲基蓝来评价BiVO4/BiPO4复合物的光催化活性.结果显示,当nV/nP<3/7的时候,BiVO4/BiPO4复合物的光催化活性随着BiVO4含量的增加而增加,当nV/nP=3/7的时候,复合物具有最佳的光催化性能,反应速率常数k为0.005 1 min-1,是纯BiPO4的23.2倍.BiVO4/BiPO4复合物的光催化机制主要是由于BiVO4的加入,提高了电子-空穴的分离率,进而提高了光催化活性.  相似文献   

5.
采用水热法合成出具有不同V、P物质的量之比的BiVO4/BiPO4复合物.nV/nP分别为:0.1/9.9、0.5/9.5、1/9、3/7、5/5.采用 XRD、FE-SEM、EDS、拉曼、可见光光度计、漫反射以及电化学等测试手段对BiVO4/BiPO4复合物进行表征.在可见光条件下降解亚甲基蓝来评价BiVO4/BiPO4复合物的光催化活性.结果显示,当nV/nP<3/7的时候,BiVO4/BiPO4复合物的光催化活性随着BiVO4含量的增加而增加,当nV/nP=3/7的时候,复合物具有最佳的光催化性能,反应速率常数k为0.005 1 min-1,是纯BiPO4的23.2倍.BiVO4/BiPO4复合物的光催化机制主要是由于BiVO4的加入,提高了电子-空穴的分离率,进而提高了光催化活性.  相似文献   

6.
以溶剂热法制备氨基功能化的Fe3O4纳米颗粒为磁核,结合溶胶-凝胶法和模板法在其表面先后包覆上致密的SiO2层和介孔TiO2层,制备了磁性-发光-微波热转换性-介孔结构为一体的多功能核-壳结构纳米复合颗粒,并对其结构、性能及载药能力进行了研究。XRD分析表明:Fe3O4表面包覆上了无定形结构的SiO2和TiO2。TEM照片表明:所得的纳米复合颗粒具有明显的核壳结构和完美的球形,构成核的Fe3O4颗粒的尺寸在40~50 nm之间,Fe3O4@SiO2@mTiO2核壳结构纳米复合颗粒的尺寸为60~70 nm,壳层厚度约10 nm,并可观察到壳层中清晰的孔状结构。磁性、荧光光谱和微波热转换特性分析表明:该复合颗粒同时具有良好的发光性、磁性和微波热转换特性。N2气吸附及药物负载率分析表明,该复合颗粒具有较高的比表面积(640 m2·g-1)和介孔结构(孔径约2.8 nm)并且具有较高的药物负载率。  相似文献   

7.
CaTiO3纳米粉体溶胶-凝胶法合成、表征及介电特性   总被引:4,自引:0,他引:4  
采用无机盐溶胶-凝胶法制备了CaTiO3纳米粉体,采用TG-DTA、XRD、TEM等技术进行了表征,并探讨了CaTiO3纳米粉体烧结特性及介电效应。结果表明,干凝胶800 ℃低温煅烧可获得粒径分布较窄、平均粒径为60~70 nm的单相CaTiO3纳米粉。纳米CaTiO3粉具有较大的比表面积,使作为粉体烧结驱动力的表面能剧增,促使CaTiO3在1 200 ℃实现致密烧结,比固相法制备的微米粉烧结降低100~200 ℃,且具有较宽的烧结温区。与微米级粉体烧结体介电特性相比,纳米粉具有更高的Qf值。纳米CaTiO3粉制备的陶瓷在1 250 ℃烧结2 h,获得优良的介电性能:εr=172,Qf=4 239 GHz,τf=+7.68 × 10-4-1。  相似文献   

8.
n型Bi2Te3-ySey温差电材料薄膜的电化学制备及表征   总被引:2,自引:0,他引:2       下载免费PDF全文
采用电化学控电位的方法在不锈钢基片上电沉积制备了Bi2Te3-ySey温差电材料薄膜。研究了电沉积溶液中硒含量与薄膜中硒含量的关系,考察了不同沉积电位对电沉积Bi2Te3-ySey薄膜的温差电性能的影响,并采用ESEM、EDS、XRD等方法对电沉积薄膜的形貌、成分及结构进行了分析。结果表明,在含有Bi3+、HTeO2+和Se4+的电沉积溶液中,采用电化学沉积的方法,可实现铋、碲、硒三元共沉积,生成Bi2Te3-ySey半导体化合物。改变电沉积溶液组成,可控制Bi2Te3-ySey化合物中硒的掺杂浓度。-0.04 V沉积电位下制备的Bi2Te3-ySey薄膜较平整、致密,组成为Bi2Te2.7Se0.3。退火处理可提高电沉积Bi2Te3-ySey薄膜的塞贝克系数,且控制沉积电位为-0.04 V下制备的Bi2Te3-ySey薄膜退火后的塞贝克系数为-123 μV·K-1。  相似文献   

9.
SrTiO3 nanorods were synthesized in cetanyl trimethyl ammonium bromide (CTAB) reverse microemulsion containing CTAB, n-hexanol, n-octane and water with Ba(OH)2 as reactants. The effects of different conditions such as ω00=nH2O/ nCTAB], aging time and the concentration of reactants on the formation of the nanorods were studied. Transmission electron microscope (TEM), electron diffraction (ED) and X-ray diffraction(XRD)were used to characterize the morphology and the structure of the synthesized nanorods. The results show that SrTiO3 nanorods with a length of 260~2 000 nm and a diameter of 50~100 nm belonging to single crystal are single cubic system. The molar ratio of Sr to Ti of products is 1.0 as determinded by ICP.  相似文献   

10.
采用固相合成法, Bi3+作施主掺杂A位, Cu2+作受主掺杂B位, 制备了Ba0.98Bi0.02(Ti0.9Zr0.1)1-xCuxO3(x=0, 0.01, 0.02, 0.03)陶瓷样品。借助XRD、LCR等研究了该陶瓷的结构与介电性能。结果表明:当x=0.03时, 陶瓷样品出现第二相。通过GULP模拟, 缺陷偶极子的稳定性从低到高依次为:[2BiBa·+VBa"]、[2BiBa·+CuTi/Zr"]、[CuTi/Zr"+VO··], 结合实验可知:介电弛豫程度与晶体中缺陷偶极子的存在形式相关, 其中x=0.01时, 晶体中以[2BiBa·+CuTi/Zr"]为主。随Cu2+掺杂量的增加, 介电常数增加, 介电常数与B位键价和呈反比变化、与八面体BO6的体积呈正比变化。  相似文献   

11.
K3InF6 is synthesized by a sol-gel route starting from indium and potassium acetates dissolved in isopropanol in the stoichiometry 1:3, with trifluoroacetic acid as fluorinating agent. The crystal structures of the organic precursors were solved by X-ray diffraction methods on single crystals. Three organic compounds were isolated and identified: K2InC10O10H6F9, K3InC12O14H4F18 and K3InC12O12F18. The first one, deficient in potassium in comparison with the initial stoichiometry, is unstable. In its crystal structure, acetate as well as trifluoroacetate anions are coordinated to the indium atom. The two other precursors are obtained, respectively, by quick and slow evaporation of the solution. They correspond to the final organic compounds, which give K3InF6 by decomposition at high temperature. The crystal structure of K3InC12O14H4F18 is characterized by complex anions [In(CF3COO)4(OHx)2](5−2x)− and isolated [CF3COOH2−x](x−1)− molecules with x=2 or 1, surrounded by K+ cations. The crystal structure of K3InC12O12F18 is only constituted by complex anions [In(CF3COO)6]3− and K+ cations. For all these compounds, potassium cations ensure only the electroneutrality of the structure. IR spectra of K2InC10O10H6F9 and K3InC12O12F18 were also performed at room temperature on pulverized crystals.  相似文献   

12.
一些具有NASICON型网格结构的固体电解质具有高的电导率和好的稳定性,NASICON的意思是Na Super Ionic Conductor[1]。当NaZr2(PO4)3中P5 被Si4 部分取代时便可以得到具有NASICON结构的Na1 xZr2SixP3-xO12体系,其具有高的钠离子电导率。然而有相同结构的Li1 xZr2SixP3-xO12体系的离子电导率却很低,这是因为Li 半径太小,而NASICON三维网格结构的离子通道太大,两者不匹配而使电导率下降[2]。但当LiZr2(PO4)3中Zr4 被离子半径小些的Ti4 取代,所得LiTi2(PO4)3的通道就与Li 半径相匹配,适合于锂离子的迁移,从而使其电导率…  相似文献   

13.
Magnetic susceptibility of Ca2F2-xMnxO5 members crystallizing in two different structures, one having octahedral (O), tetrahedral (T) and square-pyramidal (SP) coordination of transition metal atoms (OTSP structure) and the other having octahedral and tetrahedral coordination (OT structure), has been investigated. Susceptibility behaviour of the oxides with OTSP structure is different from that of the oxides with OT structure. Ca2Fe1-33Mn0-67O5 with OTSP structure shows an antiferromagnetic ordering while the corresponding oxide with OT structure shows weak ferromagnetism. Contribution No. 398 from the Solid State and Structural Chemistry Unit  相似文献   

14.
The crystal structures of Bi2.5Na0.5Ta2O9 and Bi2.5Nam-1.5NbmO3m+3 (m=3,4) have been investigated by the Rietveld analysis of their neutron powder diffraction patterns (λ=1.470 Å). These compounds belong to the Aurivillius phase family and are built up by (Bi2O2)2+ fluorite layers and (Am-1BmO3m+1)2- (m=2-4) pseudo-perovskite slabs. Bi2.5Na0.5Ta2O9 (m=2) and Bi2.5Na2.5Nb4O15 (m=4) crystallize in the orthorhombic space group A21am, Z=4, with lattice constants of a=5.4763(4), b=5.4478(4), c=24.9710 (15) and a=5.5095(5), b=5.4783(5), c=40.553(3) Å, respectively. Bi2.5Na1.5Nb3O12 (m=3) has been refined in the orthorhombic space group B2cb, Z=4, with the unit-cell parameters a=5.5024(7), b=5.4622(7), and c=32.735(4) Å. In comparison with its isostructural Nb analogue, the structure of Bi2.5Na0.5Ta2O9 is less distorted and bond valence sum calculations indicate that the Ta-O bonds are somewhat stronger than the Nb-O bonds. The cell parameters a and b increase with increasing m for the compounds Bi2.5Nam-1.5NbmO3m+3 (m=2-4), causing a greater strain in the structure. Electron microscopy studies verify that the intergrowth of mixed perovskite layers, caused by stacking faults, also increases with increasing m.  相似文献   

15.
Two new compounds, La3Ru8B6 and Y3Os8B6, were synthesized by arc melting the elements. Their structural characterization was carried out at room temperature on as-cast samples by using X-ray diffractometry. According to X-ray single-crystal diffraction results these borides crystallize in Fmmm space group (no. 69), Z=4, a=5.5607(1) Å, b=9.8035(3) Å, c=17.5524(4) Å, ρ=8.956 Mg/m3, μ=25.23 mm−1 for La3Ru8B6 and a=5.4792(2) Å, b=9.5139(4) Å, c=17.6972(8) Å, ρ=13.343 Mg/m3, μ=128.23 mm−1 for Y3Os8B6. The crystal structure of La3Ru8B6 was confirmed from Rietveld refinement of X-ray powder diffraction data. Both La3Ru8B6 and Y3Os8B6 compounds are isotypic with the Ca3Rh8B6 compound and their structures are built up from CeCo3B2-type and CeAl2Ga2-type structural fragments taken in ratio 2:1. They are the members of structural series R(A)nM3n−1B2n with n=3 (R is the rare earth metal, A the alkaline earth metal, and M the transition metal). Structural and atomic parameters were also obtained for La0.94Ru3B2 compound from Rietveld refinement (CeCo3B2-type structure, P6/mmm space group (no. 191), a=5.5835(9) Å, c=3.0278(6) Å).  相似文献   

16.
The crystal structures of compounds with nominal compositions Bi6FeP2O15+x (I), Bi6NiP2O15+x (II) and Bi6ZnP2O15+x (III) were determined from single-crystal X-ray diffraction data. They are monoclinic, space group I2, Z=2. The lattice parameters for (I) are a=11.2644(7), b=5.4380(3), c=11.1440(5) Å, β=96.154(4)°; for (II) a=11.259(7), b=5.461(4), c=11.109(7) Å, β=96.65(1)°; for (III) a=19.7271(5), b=5.4376(2), c=16.9730(6) Å, β=131.932(1)°. Least squares refinements on F2 converged for (I) to R1=0.0554, wR2=0.1408; for (II) R1=0.0647, wR2=0.1697; for (III) R1=0.0385, wR2=0.1023. The crystals are complexly twinned by 2-fold rotation about , by inversion and by mirror reflection. The structures consist of edge-sharing articulations of OBi4 tetrahedra forming layers in the a-c plane that then continue by edge-sharing parallel to the b-axis. The three-dimensional networks are bridged by Fe and Ni octahedra in (I) and (II) and by Zn trigonal bipyramids in (III) as well as by oxygen atoms of the PO4 moieties. Bi also randomly occupies the octahedral sites. Oxygen vacancies exist in the structures of the three compounds due to required charge balances and they occur in the octahedral coordination polyhedron of the transition metal. In compound (III), no positional disorder in atomic sites is present. The Bi-O coordination polyhedra are trigonal prisms with one, two or three faces capped. Magnetic susceptibility data for compound (I) were obtained between 4.2 and 350 K. Between 4.2 and 250 K it is paramagnetic, μeff=6.1 μB; a magnetic transition occurs above 250 K.  相似文献   

17.
采用水热、化学沉积和原位光还原的方法成功制备了新型Ag/Ag2MoO4/Bi2MoO6三元复合光催化剂。通过X射线粉末衍射(XRD)、扫描电子显微镜(SEM)、X射线光电子能谱(XPS)和紫外可见漫反射光谱(UV-Vis DRS)等技术对材料的组成、形貌、光吸收特性和光电化学性能等进行系统分析。以四环素为目标污染物,研究Ag/Ag2MoO4/Bi2MoO6在可见光下的光催化性能。研究结果表明,相比于纯Ag2MoO4和Bi2MoO6,Ag的表面等离子体共振(SPR)效应显著拓宽了催化体系对可见光的吸收能力及响应范围。当Ag2MoO4理论负载量(质量分数)为24.6%时,Ag/Ag2MoO4/Bi2MoO6复合材料在20 min内可将四环素完全降解,且5次循环使用后仍保持较高的催化活性,表现出良好的循环稳定性。  相似文献   

18.
采用水热合成法制备了Co3O4及复合Ag/Co3O4、CuO/Co3O4一维纳米产品。用XRD,FE-SEM和TEM手段对产品进行了表征。采用循环伏安法研究了合成产品修饰的玻碳电极在碱性溶液中对对硝基苯酚的电催化还原性能。与裸玻碳电极相比,1mmol·L-1的对硝基苯酚在用Co3O4、特别是CuO/Co3O4修饰的玻碳电极上还原的峰电流明显增大,用Ag/Co3O4(Ag/Co原子比分别为1∶5和2∶5)修饰的玻碳电极催化还原对硝基苯酚时,尽管还原峰电流增大不是太大,但其峰电位明显降低(分别降低0.265和0.371V)。  相似文献   

19.
采用水热、化学沉积和原位光还原的方法成功制备了新型Ag/Ag2MoO4/Bi2MoO6三元复合光催化剂。通过X射线粉末衍射(XRD)、扫描电子显微镜(SEM)、X射线光电子能谱(XPS)和紫外可见漫反射光谱(UV-Vis DRS)等技术对材料的组成、形貌、光吸收特性和光电化学性能等进行系统分析。以四环素为目标污染物,研究Ag/Ag2MoO4/Bi2MoO6在可见光下的光催化性能。研究结果表明,相比于纯Ag2MoO4和Bi2MoO6,Ag的表面等离子体共振(SPR)效应显著拓宽了催化体系对可见光的吸收能力及响应范围。当Ag2MoO4理论负载量(质量分数)为24.6%时,Ag/Ag2MoO4/Bi2MoO6复合材料在20 min内可将四环素完全降解,且5次循环使用后仍保持较高的催化活性,表现出良好的循环稳定性。  相似文献   

20.
A new aluminum silicon oxycarbonitride, (Al5.8Si1.2)(O1.0C3.5N1.5), has been synthesized and characterized by X-ray powder diffraction (XRPD), transmission electron microscopy (TEM), energy dispersive X-ray spectroscopy (EDX) and electron energy loss spectroscopy (EELS). The title compound is hexagonal with space group P63/mmc and unit-cell dimensions a=0.322508(4) nm, c=3.17193(4) nm and V=0.285717(6) nm3. The atom ratios of Al:Si and those of O:C:N were, respectively, determined by EDX and EELS. The initial structural model was successfully derived from the XRPD data by the direct methods and further refined by the Rietveld method. The crystal is most probably composed of four types of domains with nearly the same fraction, each of which is isotypic to Al7C3N3 with space group P63mc. The existence of another new oxycarbonitride (Al6.6Si1.4)(O0.7C4.3N2.0), which must be homeotypic to Al8C3N4, has been also demonstrated by XRPD and TEM.  相似文献   

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