硼酸镍纳米棒溶胶-凝胶法合成及表征

以硝酸镍、硼酸和柠檬酸为原料,采用溶胶凝胶法于150 ℃形成咖啡色干凝胶,再于750 ℃焙烧得到硼酸镍纳米棒。采用XRD、SEM、TEM和FTIR对产物结构和形貌进行表征。结果表明产物为分布均匀的Ni₃(BO₃)₂纳米棒,纳米棒的长度受硝酸镍和硼酸的物质的量之比影响,硼酸用量越大,长度越大。当n_Ni3(BO3)2∶n_N3BO3=1∶3时,纳米棒直径为200~300 nm,长度为2~3 μm。对硼酸镍纳米棒的生长机理进行了探讨, 结果表明, 柠檬酸与镍离子反应产生网状结构的配合物,促使镍源均匀地分散在网格间,为硼酸镍纳米棒的生成提供有利的反应空间。     

A Zigzag‐Shaped Yb4 Cluster Bridged by Pyridine‐2,6‐dimethanol

A homometallic lanthanide tetranuclear cluster, namely [Yb₄(pdmH)₂(pdm)₄ (PhCO₂)₂(PhCO₂H)₂(H₂O)₂] · PhCO₂H · 0.25MeOH ( 1 ) (pdmH₂ = pyridine‐2,6‐dimethanol) was prepared and structurally characterized. Single‐crystal X‐ray analysis revealed that complex 1 has a tetranuclear core with a zigzag arrangement. Magnetic properties of complex 1 were also investigated.     

双柱双检测器气相色谱法同时进样分析非甲烷烃的不确定度

双柱双检测器气相色谱法同时进样分析非甲烷烃,对甲烷、总烃、氧气和仪器引入的不确定度进行了评定.结果显示,本法测定不确定度的主要来源为标准气体的不确定度,其次是色谱分析仪器引入的不确定度,相对分子质量引入的不确定度可忽略不计.环境空气中非甲烷烃测定结果为(0.85±0.14)mg/m<'3>,k=2.     

约束向量优化问题的Fenchel-Lagrange对偶及鞍点

The aim of this paper is to apply a perturbation approach to deal with Fenchel- Lagrange duality based on weak efficiency to a constrained vector optimization problem. Under the stability criterion, some relationships between the solutions of primal problem and the Fenchel-Lagrange duality are discussed. Moreover, under the same condition, two saddle-points theorems are proved.     

Investigation of scatter from out of the field of view and multiple scatter in PET using Monte Carlo simulations

In fully three-dimensional (3D) positron emission tomography (PET) imaging, the scatter fraction (SF) is about 40%-60%, which may degrade the imaging quality severely. Scatter correction is important for high quality image reconstruction. Model-based scatter correction has been proved to be accurate and available in clinical PET. However, it does not correct the scatter from out of the field of view (OFOV) and multiple scatters. In this study, we demonstrate the radial and axial distribution of scatters from OFOV when the source is located in different radial positions. In order to apply the above conclusions to different PET systems, we characterize the scatters from OFOV as a function of the ratio of the scanner diameter to the length of the axial field of view (AFOV) by modeling several typical whole-body and micro PET systems. The proportions of true events (S_0-0), single scatter of one photon (S_1-0) , single scatter of both photons (S_1-1) , double scatter of one photon (S_2-0) and multiple scatter (S_m) are also calculated and compared. Here the 3D-PET Monte Carlo simulations are performed with the Geant4 Application for Tomography Emission (GATE). In summary, the scatters from OFOV tend to be recorded on the lines of response (LOR) far away from the source. They have a much more serious impact on whole-body PET than micro PET depending on the ratio of scanner diameter to the length of AFOV. In whole-body PET, twice scatters including single scatter of both photons (S_1-1) and double scatter of one photon (S_2-0) add up to about 12% so that twice scatter correction must be taken into account to acquire a high quality reconstruction image.     

Synthesis and characteristics of natural zeolite supported Fe-TiO2 photocatalysts

Natural zeolite supported Fe³⁺-TiO₂ photocatalysts were synthesized for the sake of improving the recovery and photocatalytic efficiency of TiO₂. The as-prepared materials were characterized by X-ray diffraction (XRD), fourier transform infrared spectroscopy (FT-IR), X-ray photoelectron spectroscopy (XPS), ultraviolet-visible diffuse reflection spectroscopy (UV-vis DRS), scanning electron microscopy (SEM) and energy-dispersive X-ray analysis (EDX). Methyl orange was used to estimate the photocatalytic activity of the samples. The results showed that zeolite inhibited the growth of TiO₂ crystallite sizes. The Fe³⁺ concentration played an important role on the microstructure and photocatalytic activity of the samples. The iron ions could diffuse into TiO₂ lattice to the form Fe-O-Ti bond and gave TiO₂ the capacity to absorb light at lower energy levels. The photocatalytic activity of the samples could be enhanced as appropriate dosages of Fe³⁺ were doped.     

Fast epitaxial growth of a-axis- and c-axis-oriented YBa2Cu3O7−δ films on (1 0 0) LaAlO3 substrate by laser chemical vapor deposition

a-axis- and c-axis-oriented YBa₂Cu₃O_7−δ (YBCO) films were epitaxially grown on (1 0 0) LaAlO₃ substrates by laser chemical vapor deposition. The preferred orientation in the YBCO film changed from the a-axis to the c-axis with increasing laser powers from 77 to 158 W (the deposition temperatures from 951 to 1087 K). The a-axis-oriented YBCO film showed in-plane epitaxial growth of YBCO [0 0 1]//LAO [0 0 1], and the c-axis-oriented YBCO film showed that of YBCO [0 1 0]//LAO [0 0 1]. A c-axis-oriented YBCO film with a high critical temperature of 90 K was prepared at a deposition rate of 90 μm h⁻¹, about 2-1000 times higher than that of metalorganic chemical vapor deposition.     

毫米波辐照下大鼠脑电的长程相关性

通过脑电长程相关性的分析,定量研究了35 GHz毫米波辐照大鼠时产生的应激反应.通过退趋势分析法,得到反映高频成分的标度指数.显示在辐照前该成分具有布朗噪声的特性,辐照时具有长程相关性;而反映低频成分的标度指数显示在辐照前该成分具有长程相关性,辐照时成为布朗噪声.引进应激指标参量低频成份标度指标数/高频成份标度指标数,...     

Tunability and linewidth sharpening of plasmon resonances on a periodic gold nanowire array coupled to a thin textured silver film

We theoretically study the plasmon mode spectrum of a multilayer structure consisting of a periodic gold nanowire array and a spatially separated thin silver film with periodic slits. Results show that the plasmon mode spectrum of the multilayer structure depends sensitively on the relative lateral displacement of the Au nanowire array with respect to the textured silver film. This is due to the interaction between the localized surface plasmon (LSP) of the nanowire array and the plasmon modes, including the horizontal LSP and the antisymmetric short-range surface plasmon polariton (SPP), of the textured thin silver film. The strong coupling between the LSP and the antisymmetric short-range SPP results in a redshifted plasmon resonance with a significantly narrow linewidth and a large electromagnetic field enhancement. Moreover, the lateral displacement also has a great influence on the spacer layer controlled dipole-surface interaction. Therefore, this relative lateral displacement provides an efficient way to tune the optical properties of the multilayer structure, and this kind of highly tunable nanostructure can be used as a tunable plasmonic filter or a substrate for LSPs sensor.