Aligned CuO nanorod arrays: fabrication and anisotropic ferromagnetism

Copper oxide (CuO) is a p-type semiconductor with a band gap of 1.2 eV, which is well known in high-temperature superconductor and antiferromagnetic (AFM) materials through Cu–O–Cu super-exchange interaction. In this paper, we report the strong anisotropic ferromagnetism (FM) in aligned CuO nanorod arrays synthesized by a microwave-assisted hydrothermal method. The transmission electron microscopy (TEM) image shows that the CuO nanorod consists of a large number of smaller nanorods with almost the same growth direction. The X-ray diffraction (XRD) pattern indicates that the CuO nanorods are well crystallized with highly preferred orientation of the [020] direction. These CuO nanorod arrays show room-temperature ferromagnetism, with strong magnetic anisotropy when the magnetic field is applied perpendicular or parallel to the rod axis. This phenomenon of room-temperature ferromagnetism in those aligned CuO nanorods might originate from uncompensated surface spins and shape anisotropy of the nanorods.     

Model for spontaneous frequency sweeping of an Alfvén wave in a toroidal plasma

We study the frequency chirping signals arising from spontaneously excited toroidial Alfvén eigenmode (TAE) waves that are being driven by an inverted energetic particle distribution whose free energy is tapped from the generic particle/wave resonance interaction. Initially a wave is excited inside the Alfvén gap with a frequency determined from the linear tip model of Rosenbluth, Berk and Van dam (RBV) [1]. Hole/clumps structures are formed and are observed to chirp towards lower energy states. We find that the chirping signals from clump enter the Alfvén continuum which eventually produce more rapid chirping signals. The accuracy of the adiabatic approximation for the mode evolution is tested and verified by demonstrating that a WKB-like decomposition of the time response for the field phase and amplitude agree with the data. Plots of the phase space structure correlate well with the chirping dependent shape of the separatrix structure. A novel aspect of the simulation is that it performed close to the wave frame of the phase space structure, which enables the numerical time step to remain the same during the simulation, independent of the rest frame frequency.     

Further results on stabilization of neural-network-based systems using sampled-data control

Nonlinear Dynamics - This paper investigates the problem of stabilization for sampled-data neural-network-based systems under variable sampling. A novel Lyapunov–Krasovskii functional (LKF)...     

Existence results for second-order system with impulse effects via variational methods

In this paper, we investigate the positive solutions of a second-order system with impulse effects. By using critical point theory the existence result of positive solutions is obtained.     

M2+(M=Cu、Cd、Ag、Fe)掺杂氧化锌纳米粉晶的抗菌性能

采用柠檬酸溶胶-凝胶法制备了ZnO及M²⁺掺杂ZnO纳米粉晶(M=Cu、Cd、Ag、Fe),用现代测试技术表征了样品的组成、结构和形貌,以大肠杆菌(Escherichia coli)、金黄色葡萄球菌(Staphylococcus aureus)和白色念珠菌(Candida albicans)为测试菌株,用抑菌圈、最小抑菌浓度和最小杀菌浓度等方法研究了样品在日光照射下的抗菌活性。结果表明,与母体ZnO相比,Cu、Ag、Cd掺杂样品的抗菌性能明显地增强,这可能是由于掺杂金属离子置换Zn²⁺生成了晶格缺陷和电荷缺陷,阻止了光生电子和光生空穴对的复合从而增强了光催化活性和抗菌活性。     

水热法制备Pr掺杂Bi2WO6三维花状微球的光催化性能

通过水热法制备稀土Pr掺杂Bi₂WO₆三维花状微球,利用XRD、SEM、N₂吸附-脱附、紫外-可见吸收光谱和光致发光光谱对所制备的光催化材料进行表征。通过降解亚甲基蓝评价样品的光催化活性。结果表明,1.0% Pr-Bi₂WO₆样品的可见光催化活性最佳,降解率达到95%。Pr掺杂提高了催化剂的可见光吸收性能并且能够束缚光生电子使得电子空穴对有效分离从而获得强氧化物质。对其光催化降解做出了合理的解释。     

两个苯甲羟肟酸有机锡配合物的合成、结构及抗癌活性

合成了2个苯甲羟肟酸有机锡配合物：[(o-Cl-C₆H₄CH₂)₂Sn (C₆H₅CONO)₂](1)和[(o-CH₃-C₆H₄CH₂)₂Sn (C₆H₅CONO)(C₆H₅COO)](2)。通过元素分析、红外光谱、核磁共振氢谱、热重分析、单晶X射线衍射等方法对配合物进行了结构表征,对其结构进行量子化学从头计算和体外抗癌活性研究。结果显示：配合物均为单锡核结构,配合物1为六配位的畸变八面体构型,配合物2为五配位的畸变三角双锥构型;配合物1对人宫颈癌细胞(HeLa)、肝癌细胞(HuH-7)和肺腺癌细胞(H1975)显示出比临床使用的顺铂强的抑制活性,而配合物2的抑制活性要弱得多。     

中枢多巴胺系统正电子发射计算机断层扫描显像剂的研究进展

中枢多巴胺系统与多种神经行为障碍的病理生理学有关。一直以来,多巴胺系统正电子发射计算机断层扫描(PET)成像在研究活体大脑中多巴胺生物化学过程上有着重要价值。PET成像的基础是¹¹C、¹⁸F等发射正电子的放射性核素标记的显像剂,这些显像剂通过与多巴胺神经系统不同的靶点特异性结合从而反映多巴胺合成、囊泡储存、突触释放和受体结合以及再摄取过程,推动神经病学、精神病学、药物滥用和成瘾以及药物开发的研究进展。本文综述了以氨基酸脱羧酶、多巴胺转运体、多巴胺受体以及囊泡单胺转运体为靶点的¹¹C、¹⁸F标记的PET显像剂的研究进展。