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合成了组成为(Y,Zn,Sr)3(P,VO4):Eu^3+,Bi^3+的荧光材料,经X射线结构分析确定为Zn3(PO4)2结构,属于单斜晶系,空间群为P21/n。讨论了基质组成对Eu^3+离子发光性质的影响,用Y^3+取代了一部分Zn^2+;用VO4取代了一部分PO4由于基质的436nm发射与Eu^3+的激发态能级的能量重叠,Eu^3+产生较强的598nm和618nm发射。另外,掺入少量Bi^3+  相似文献   

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《照相机》2002,(6)
本刊讯 美能达公司推出准专业级的α-7和摄影爱好者最佳柏挡α-5之后,深受广大用户的好评。近期,公司又推出了一款性价比相当高的普及型入门相机美能达α-3,α-3继承了美能达一贯推崇的产品理念,  相似文献   

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Crystals of the rare-earth gallium borates RGa3(BO3)4, where R = Nd, Sm–Er, or Y, were grown by the flux method. The crystal structures of RGa3(BO3)4 (R = Eu, Ho) were studied on the basis of single-crystal X-ray diffraction measurements. The hexagonal unit-cell parameters are a = 9.4657(1) Å, c = 7.4667(1) Å and a = 9.4394(2) Å, c = 7.4322(1) Å for EuGa3(BO3)4 and HoGa3(BO3)4, respectively, space group R32. Structure model was determined by “charge flipping” method and refined to R = 1.93% [EuGa3(BO3)4] and R = 1.89% [HoGa3(BO3)4] in anisotropic approximation. All grown gallium borates were investigated by infrared (IR) spectroscopy technique in a middle and far IR region. IR spectra of rare-earth gallium borates correspond to a pure rhombohedral (R32) polytype structure. Small inclusions of a monoclinic phase were detected only in Eu and Nd compounds. Luminescence of Eu and Ho gallium borates was studied at room temperature. The measured decay times for the most intensive emission lines of EuGa3(BO3)4 (∼614 nm) and HoGa3(BO3)4 (434 nm) are 940 μs and 140 μs, respectively. The scheme of crystal-field energy levels of Eu3+ in EuGa3(BO3)4 was built on the basis of the temperature-dependent optical transmission measurements combined with the luminescence data. The measured UV absorption edge for RGa3(BO3)4 is at about 300 nm.  相似文献   

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LaFe0.9Mn0.1O3?δ and LaFeO3 were synthesized and characterized by X-ray powder diffraction, scanning electron microscopy, Fourier transform infrared, XPS techniques, UV–Visible absorption spectra techniques, vibrating sample magnetometer, and room temperature Fe57 Mössbauer spectra. They were also evaluated for their photocatalytic activity toward the degradation of methyl orange under the sunlight irradiation. The experimental results show that the catalytic activities of the Mn-doped in LaFeO3, i.e., LaFe0.9Mn0.1O3?δ were much higher than those of LaFeO3 due to its higher oxygen vacancies, variable valency Mn ions and the strong absorption in visible light, and it has higher magnetic property than that of LaFeO3 due to the existence of Mn3+/Fe3+and Mn3+/Mn4+double exchange interaction in LaFe0.9Mn0.1O3?δ. The LaFe0.9Mn0.1O3?δ is the photocatalyst with intrinsic magnetic property and visible light activity, and it is applicable to the magnetic separation process for its higher saturated magnetization (M s), lower coercivity (H c), and remanent magnetization (M r) as well as the superparamagnetic contribution in the sample, and it can be reusable and maintain relatively high activity.  相似文献   

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Journal of Materials Science: Materials in Electronics - The impact of Zn substitution on structural, dielectric, and reflection properties of the pure MgTiO3 and 0.96 ZnxMg1?xTiO3–0.04...  相似文献   

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<正>"我们的技术将在先进制造领域掀起新一轮的革命。"日前,华中科技大学机械科学与工程学院教授张海鸥携其研发的"智能微铸锻铣复合制造技术",与法国空客公司举行了技术合作签约仪式,这是法中两国在先进制造领域的一项重要合作。这位年过60岁的老人和夫人王桂兰一起,带领团队用14年的时间,破解了困扰金属3D(三维)打印的世界级技术难题,实现了我  相似文献   

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Data are presented on the phase transitions and physical properties of K3Nb3B2O12 (KNB) and K3 – Na x Nb3B2O12 (KNNB) crystals. Detailed measurements of the dielectric permittivity, nonlinear optical properties, and electrical conductivity, as well as examination of the domain structure, demonstrate that KNB and KNNB exhibit a complex polymorphism: both have eight different polymorphs between –100 and 900°C. The introduction of Na into KNB raises the transition temperatures, which makes it possible to investigate the low-temperature phases at room temperature. The high-temperature phase transition is antiferroelectric, whereas the other transitions are of a ferroelectric–ferroelastic nature. Along with complex polymorphism, KNB and KNNB exhibit superionic conductivity.  相似文献   

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The growth pressure-temperature region of cubic boron nitride (cBN) in the systems Mg-BN and MxNy-BN (MxNy=Li3N, Ca3N2, Mg3N2) has been redetermined using well-crystallized hexagonal BN (hBN) with low oxygen content (0.2%) as the starting material. The data on the MxNy-BN systems are compatible with the existence of two growth regions: a high-temperature region where cBN grows from a liquid phase, and a low-temperature region where cBN forms from solid-solid reactions. Previous data are discussed according to this model and possible solid-state reactions are proposed on the basis of thermodynamic considerations. The results for the Mg-BN system confirm the effect of the O2 content of the starting BN on the cBN growth region. The systems (MxNy + M)-BN (M=Al, B, Si, Ti) have been shown to produce cBN crystals of increased size and improved morphology (more compact and perfect) compared to those obtained with the MxNy-BN systems. Their colour is dark or black and their size reaches 0.6 mm. The effect of the relative proportions of M and MxNy on the growth region and yield has been determined and is discussed on the basis of the chemical reactions likely to occur.  相似文献   

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Highly pure butterfly-shaped BiFeO3@BaTiO3 nanotubes have been synthesized through a sol–gel method. An obvious ferromagnetic behavior was obtained at room temperature, with a large coercive field (5,403 Oe) and high Mr/Ms value (0.52). The dielectric permittivity of BiFeO3@BaTiO3 nanotubes was found to be 1919, which is much higher than that of pure BFO nanostructure. The dielectric loss of BiFeO3@BaTiO3 nanotubes is low in the frequency range from 10 Hz to 1 MHz. The maximum magnetoelectric coefficient of BiFeO3@BaTiO3 nanotube is 0.272 μV/cm Oe. Moreover, the BiFeO3@BaTiO3 nanotubes have exhibited a better ferroelectric property with a large band gap of 3.2 eV which demonstrates the core–shell nanostructure.  相似文献   

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Multiferroic nanomaterials have attracted great interest due to simultaneous two or more properties such as ferroelectricity,ferromagnetism,and ferroelasticity,which can promise a broad application in multifunctional,lowpower consumption,environmentally friendly devices.Bismuth ferrite(BiFeO3,BFO)exhibits both(anti)ferromagnetic and ferroelectric properties at room temperature.Thus,it has played an increasingly important role in multiferroic system.In this review,we systematically discussed the developments of BFO nanomaterials including morphology,structures,properties,and potential applications in multiferroic devices with novel functions.Even the opportunities and challenges were all analyzed and summarized.We hope this review can act as an updating and encourage more researchers to push on the development of BFO nanomaterials in the future.  相似文献   

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Ln-doped Sb2Te3 (Ln: Lu3+, Er3+, Ho3+) nanomaterials were synthesised by a co-reduction method in hydrothermal condition. Powder X-ray diffraction (XRD) patterns indicate that the LnxSb2?xTe3 crystals (Ln = Lu3+, x = 0.00–0.06; Er3+ and Ho3+ x = 0.00–0.04) are isostructural with Sb2Te3. The cell parameter a decreases for LnxSb2?xTe3 compounds upon increasing the dopant content (x), while c increases. Scanning electron microscopy and transmission electron microscopy images show that doping of Lu3+ and Ho3+ ions in the lattice of Sb2Te3 results in spherical nanoparticles while that in Er3+ leads to hexagonal nanoplates, respectively. The electrical conductivity of Ln-doped Sb2Te3 is higher than that of pure Sb2Te3 and increases with temperature. By increasing the concentration of Ln3+ ions, the absorption spectrum of Sb2Te3 shows red shifts and some intensity changes. In addition to the characteristic red emission peaks of Sb2Te3, emission spectra of doped materials show other emission bands originating from ff transitions of the Ho3+ ions.  相似文献   

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The crystal structure of 3, 3′-dimethoxybiphenyl has been determined by X-ray diffraction methods with an aim of describing the hydrogen interaction in biphenyl derivatives. The title compound crystallizes in monoclinic space groupP21/c with unit cell dimensions,a = 7.706(1),b = 11.745(2),c = 12.721(2) Å, β = 92.31(1)°,Z = 4 and its structure has been refined up to the reliability index of 3.8%. The average torsion angle about the inter-ring C-C bond is 37.5°. The O1 and Ol′ atoms of the methoxy group are deviated by 0.046(1) Å and 0.234(1) Å from the mean planes of respective rings. The crystal cohesion is pronounced due to three-inter-molecular C-H...O hydrogen bonds.  相似文献   

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