Effect of Al^3＋ on Photoluminescence Properties of Eu^3＋-Doped BaZr（BO3）2 Phosphors

We discuss the influence of Al^3＋ on the charge transfer state （CTS） and the photoluminescence properties of BaZr（BO3）2：Eu. The results reveal that there is a red shift which is about 20nm for the charge transfer state when doping with Al^3＋ and indicate the formation of ‘free＇ electrons due to the change of microstructures. In addition, the influence or Al^3＋ doping on the PPR is analysed and a new explanation is raised based on the photo luminescent mechanism. It is the CTS intensity rather than the CTS energy that influences the peak-peak ratio.     

Intercalation Reaction of Bi2(Sr,Nd)2CuOyBi2Sr2(Ca,Gd)Cu2Oy and Related Compounds with Iodine

With iodine vapour treatment of various single crystals of Bi-Sr-Ca-Ln(Rare earch element)-Cu-O system, the stage-1 iodine-intercalation compounds of Bi₂(Sr,Nd)₂CuO_y(2201), Bi₂Sr₂(Ca,Gd)Cu₂O_y or Bi₂Sr₂CaCu₂O_y(2212) and Bi₈SrCaO₁₄ have been prepared. x-ray diffraction and transmission electron microscope analysis indicate that iodine layer of thickness 3.2～3.5Å is formed between two Bi₂-O₂     

Magnetic Force Microscopy Study of Alternate Sputtered （001） Oriented L1o Phase FePt Films

We present a magnetic force microscopy study of alternate sputtered （001） oriented L1o phase FePt films. It is found that the root-mean-square value of phase shift of magnetic force images, （ △Ф）rms, can be used to characterize the perpendicular anisotropy for a series of specimens. Therefore, the considerable improvement of the perpendicular anisotropy after post-annealing can be characterized. In addition, the magnetic properties, magnetic and crystalline microstructures before and after post-annealing are compared for the typical [Fe5nm Pt5 nm]10 film with substrate temperature T8 = 500℃, single layer thickness d = 5 nm and total layer thickness D=100 nm to confirm the effect of post-annealing on improving the perpendicular anisotropy for Fe-Pt films.     

Gaseous Hydrogenation and Its Effect on Thermal Stability of Mg63Ni22Pr15 Metallic Glass

Mg63Ni22Pr15 metallic glasses are produced by a single roller melt-spinning technique. The hydrogen absorption and desorption capacities are respectively 0.38 and 0.14 wt% at 313 K obtained by pressure-composition isotherm. The amorphous structure is found to be retained after gaseous hydrogenation. The glass transition temperature, the onset crystallization temperature, and the crystallization temperature of the hydrogenated Mg63Ni22Pr15 metallic glass are 550, 570 and 577K, respectively, much higher than the corresponding values of 440, 470 and 499K of the as-quenched sample. This means that dramatic enhancement of thermal stability occurs in Mg63Ni22Pr15 metallic glass due to hydrogenation.     

Photocatalytic Properties of TiO2/Si-NPA Nano Composite Systems

A new composite system is fabricated by depositing the TiO2 film on a silicon nanoporous pillar array （Si-NPA） and annealing at 500℃ using the spin coating method. Such a composite system exhibits a uniform morphology with the micron-dimension pillar array. Photocatalytic properties are investigated based on the degradation of methyl orange dye solution, and the results show that the photocatalytic efficiency of such a nano-composite system is 1.7 times that of the TiO2/glass system. The enhancement of photocatalytic efficiency is attributed to the large surface area of the TiO2/Si-NPA system.     

Magnetic structure of geometrically frustrated compound Co2Cl(OH)3 determined by proton NMR

The magnetic structure of a geometrically frustrated system Co₂Cl(OH)₃ is determined by comparing the observed proton NMR spectrum with numerical calculations based on various magnetic models. The best fit is obtained with a model that the magnetic moments of Co²⁺ ions in the triangular plane are parallel to the principal axis of local crystal field and those of Co²⁺ ions in the kagome lattice plane are randomly disordered in the a-b plane, which nearly bisects the angle between the principal axis of the local field and a line pointing towards the body center of the tetrahedron. The coexistence of the ferromagnetic order in the triangular plane and the random disorder in the kagome plane is consistent with the results of measurements by Zheng et al. However, the magnetic moments of Co²⁺ ions are not directed towards the body center of the tetrahedron as characteristic in the “spin ice” magnetic structure. Furthermore, the Co²⁺ ions in the triangular plane have a smaller magnitude of magnetic moment than those in the kagome plane. Thus, our result suggests that the transition metal compound Co₂Cl(OH)₃ is different from the “spin ice” in magnetic structure, although it is similar to rare-earth pyrochlores in crystal structure.     

Analysis of （1, 2） （1, 3） and （2, 3） Bands in the c^3Ⅱu- b^3Ⅱg System of P2

We investigate the high resolution absorption spectroscopy of P2 radical, generated in ac glow discharge of PC13 buffered with helium, using optical heterodyne magnetic rotation enhanced concentration modulation spectroscopy in the visible region. The （1, 2）, （1, 3） and （2, 3） bands of c^3Ⅱu- b^3Ⅱg in the range 16620-17860cm^-1 are observed and their 3II2 3II2 subbands are rotationally analysed. A set of effective molecular constants for the Ω= 2 component of the states involved are determined.     

Magnetic properties of the bilayer manganese oxide (Pr0.6La0.4)1.2Sr1.8Mn2O7 under pressure

We investigated the effect of pressure on the magnetic properties of a single crystal of the bilayer manganese oxide (Pr_0.6La_0.4)_1.2Sr_1.8Mn₂O₇ by means of DC magnetization measurements under pressure. The ferromagnetic transition, which is accompanied by a metal-insulator transition, is highly sensitive to pressure. The pressure causes a structural variation, which affects the magnetic properties. We discuss the pressure dependence of the 3d electronic state of the Mn ion in this system.     

Magnetic characteristics of hyperstoichiometric ZrCrFeT0.8 (T = Mn,Fe, Co and Ni) and hydrides

Magnetic behavior has been established for the hypertoichiometric ZrCrFeT_0.8 (T = Mn, Fe, Co and Ni) systems and their hydrides as well as stoichiometric ZrCrFe and its hydride at temperatures extending from 4 to 1200 K and at field strengths up to 20 kOe. All systems possess the hexagonal Laves structure (C14). Long-range magnetic ordering appears to be absent in the parent systems. ZrCrFe, ZrCrFeMn_0.8 and ZrCrFe_1.8 exhibit spin-glass-like behavior. In all systems hydrogenation is accompanied by a large expansion of volume, ranging from ≈ 20% to ≈ 30%, with no change in crystal structure. Upon hydrogenation long-range ferromagnetism appears in ZrCrFe and ZrCrFe_1.8 but not in the other ZrCrFeT_0.8 systems. The onset of the long-range magnetic ordering is interpreted in terms of the formation of ferromagnetic clusters of Fe.     

Influence of MNi2 (M=Sc,Y, La,Lu) compounds on the ferromagnetism of HoNi2–MNi2 solid solutions

Ferromagnetic properties of HoNi₂–MNi₂ solid solutions were studied. HoNi₂ is a typical rare earth ferromagnet with the Curie temperature equal to 17.6 K. The source of ferromagnetic order are exchange interaction between magnetic moments of holmium atoms. In the case of solid solutions HoNi₂–MNi₂ for M=Sc, Y and La, the disappearance of ferromagnetic order has been observed for concentrations of M higher than 60 atomic % whereas for the system HoNi₂–LuNi₂ the ferromagnetic order is observed even in Lu_0.80Ho_0.20Ni₂ solid solution. Values of the magnetic saturation moment μ_s for M_xHo_1−xNi₂ solid solutions with x?0.60 are close to the value of μ_s of undiluted HoNi₂. Moreover, the value of μ_s of HoNi₂ suggests that, apart from the contribution of holmium a small contribution of Ni atoms is added. The paramagnetic Curie temperatures Θ are somewhat lower than the values typical of ferromagnets: usually Θ is almost equal to T_C. Paramagnetic moments of the solid solutions are similar or higher than that found for pure HoNi₂. On the basis of the results obtained one may have to state that the influence of the LuNi₂ is the weakest and this compound may be regarded as the best diluter and, in the case of heat capacity measurements, also as the best reference material.