Electron Magnetohydrodynamics Magnetic Reconnection Experiment on Keda Linear Magnetized Plasma Device

We conduct an electron magnetohydrodynamics magnetic reconnection experiment with guide-field in our Keda linear magnetized plasma device, in which two pulsed currents with the same direction are conducted in parallel with the axial direction of the main chamber of the device using two long aluminum sticks. After approximately 5μs, an X-type magnetic field line topology is formed at the center of the chamber. With the formation of the X-type topology of magnetic field lines, we can also find the rapid increase of the current and ratio of the common flux to the private flux in this area. Additionally, a reduction in the plasma density and the plasma density concentration along one pair of separatrices can also be found.     

发光材料BaAl2Si2O8∶Eu^2＋的物相结构与发光性能

硅酸盐类物质作为发光材料基质．发光中心和基质相互作用能量较低。可使发光中心离子直接吸收激发能量,利于提高发光效率。目前。研究较多的硅酸盐类发光材料为Zn2SiO4、Sr2MgSi2O7、Ba3MgSi2O8等。铝硅酸钡通常归属于硅酸盐范畴,铝硅酸盐的结构复杂、物相组成变化多样．一般实验条件下很难获得单一物相产物。碱土金属铝硅酸盐作为发光材料基质由来已久,     

发光材料BaAl2Si2O8∶Eu2+的物相结构与发光性能

A phosphor, Ba_0.97Al₂Si₂O₈∶Eu²⁺, was synthesized by high temperature solid-phase method at different temperatures. The samples were characterized by TG/DTA, XRD and fluorescence spectroscopy. The results show that the main phase for host of these luminescence materials is barium feldspar BaAl₂Si₂O₈∶Eu²⁺ and there is a transition from hexagonal crystal system to monoclinic crystal system in the process of the sintering of barium feldspar. The luminescent phenomen of barium feldspar with hexagonal structure can not be observed under the excitation of ultraviolet lamp of 365 nm while the barium feldspar with monoclinic structure has excellent luminescence properties. The excitation spectra of all these samples show broad band spectra ranging from 250～390 nm with peak at λ_ex of 357 nm,which indicates that these samples can be effectively excited by near ultraviolet ; the emission spectra range from 380～600 nm with peak at λ_em of 433 nm. The luminescent intensity increases then decreases with the concentration of doping Eu²⁺ ions. When the concentration of dopants is 2.5mol%, the luminescent intensity reaches the maximum value. When the concentration of Eu²⁺ ions changes from 0.5mol% to 2.5mol%, the emission peak has a red shift from 427 nm to 440 nm.