High-Pressure Phase Transition in Cyclo-octane

Structural behaviour of cyclo-octane under high pressure is studied by using a synchrotron x-ray source in a diamond anvil cell （DAC） up to 40.2 GPa at room temperature. The cyclo-octane firstly solidifies to the triclinic phase at 0.87 GPa. With the increasing pressure, the phase of cyclo-octane changes to the tetragonal phase at about 6.0 GPa and then transforms to amorphous phase above 18.2 GPa, which is kept till to 40.2 GPa. All the phase transitions of cyclo-octane are irreversible.     

High-Pressure Phase Transitions of Cubic Y_2O_3 under High Pressures by In-situ Synchrotron X-Ray Diffraction

High-pressure phase transitions of cubic Y_2O_3 are investigated using in situ synchrotron x-ray diffraction in a diamond anvil cell up to 36.3 GPa. The pressure-induced phase transitions of cubic Y_2O_3, which display apparent inconsistencies in previous studies, are verified to be from a cubic phase to a monoclinic phase and further to a hexagonal phase at 11.7 and 21.6 GPa, respectively. The hexagonal Y_2O_3 displays noticeable anisotropic compressibility due to its layered structure and it is stable up to the highest pressure in the present study. A third-order Birch–Murnaghan fit based on the observed pressure-volume data yields zero pressure bulk moduli of180(3), 196(7) and 177(7) GPa for cubic, monoclinic and hexagonal phases, respectively.     

不同粒径纳米晶硫化锌的高压结构相变研究

 应用原位能量色散X射线散射和金刚石对顶砧技术，对纳米晶ZnS进行了高压结构相变研究。初始相为纤锌矿结构的10 nm和3 nm硫化锌分别在16.0 GPa和16.7 GPa时转变为岩盐矿结构，相变压力均高于纤锌矿结构的体材料硫化锌。该相变为一可逆的结构相变。应用大型科学计算软件Materials Studio（MS）计算了纳米晶ZnS的状态方程，根据Birch-Murnaghan方程拟合了纳米晶ZnS的零压体模量，得到的零压体模量高于相应体材料的零压体模量，表明纳米晶ZnS较难压缩。     

氧化镓的同步辐射研究

 利用金刚石对顶砧（DAC）高压装置产生高压，使用体积比为16∶3∶1的甲醇、乙醇和水混合液作为传压介质，通过原位高压同步辐射技术对氧化镓的高压行为进行了研究（0～42.5 GPa）。实验发现在室温下13.3 GPa压力附近，单斜结构的氧化镓发生了结构相变，变成三角结构。相变后镓离子由原来同时位于由氧离子围成的四面体和八面体的中心位置变成只位于八面体的中心位置。卸压后的X射线衍射谱表明，氧化镓又恢复为单斜结构，该相变为可逆相变。     

Mn3Zn0.8Ni0.2N的高压同步辐射研究

 利用金刚石对顶压砧,对钙钛矿型金属锰化物Mn₃Zn_0.8Ni_0.2N进行了原位高压同步辐射角散X射线衍射研究。研究表明,在0~29.9 GPa的压力区间内,样品没有发生结构相变,因而在该压力下样品的物性变化并非由结构相变所导致。卸压以后,样品的特征峰都回到了初始位置。通过Birch-Murnaghan方程,拟合得到了样品的体弹模量为86.5 GPa。     

层状钙钛矿结构锰氧化物Ca3Mn2O7的压致结构相变

采用金刚石压砧高压装置(DAC),对层状钙钛矿结构锰氧化物Ca     

Phase Transition of Graphitic-C3N4 under High Pressure by In Situ Resistance Measurement in a Diamond Anvil Cell

In situ resistance measurement of Graphitic-C3N4 has been performed under high pressure in a diamond anvil cell. The result reveals that there are changes of electron transport behaviour. As the pressure increases from ambient to 30 GPa, three abnormal resistance changes can be found at room temperature and two are found at 77K. The abnormal resistance dropped at 5 GPa is close to the phase transition pressure from the P6m2 structure to the p structure predicted by Lowther et al. [Phys. Reg. B 59 (1999) 11683] Another abnormal change of resistance at 12 GPa is related to the phase transition from g-C3N4 to cubic-C3N4 [Teter and Hemley, Science 271 (1990) 53].     

竹红菌甲素的光化学——甲素敏化的烯烃光氧化反应的研究——甲素产生~1O_2的作用

本文研究了甲素敏化的烯烃光氧化反应,证实了甲素有产生~1O_2的作用。测定了甲素敏化的~1O_2的量子产率,还研究了甲素敏化的反式芪的光氧化反应。分离并鉴定了产物。主产物为1-苯甲酰甲叉-2,5-过氧桥-6-羟基环己烯-3及它的异构体。结果表明,可能是经由双桥环过氧化物(diendoperoxide)的质子重排得到的。在这个反应中,活泼态的氧对苯乙烯的1.4-环加成占优势,这是一个新结果。     

Equation of State of Tantalum up to 133GPa

The static equation of state （EOS） of tantalum （Ta） is determined by in situ energy-dispersive synchrotron powder x-ray diffraction in a diamond anvil cell （DAC） up to 133GPa. The body-centered-cubic （bcc） phase of Ta is found to be stable over the entire pressure range investigated. The bulk moduli and its first pressure derivative of Ta are constrained by fitting the determined pressure-volume data to Vinet form EOS： B0 =192.65±（3.08）GPa and B＇0 =3.58±（0.11）. For the sake of avoiding the affect of non-hydrostatic stress, argon is used as a pressure media. A careful checking of the stress state of the sample is presented simultaneously.     

纳米脂质体复合物-包封多酸化合物的合成,表征和生物活性研究

The polyoxometalate K6H[CoW11O39（CpTi）] （abbreviated as CoW11CpTi, Cp=η^5-C5H5） loaded nanosize-liposome complex has been prepared and structurally characterized by elemental analysis, IR and UV spectra. The particle size of the complex was distributed in the range of 100-250 nm with the average diameter of 132.6 nm. The result showed that the polyoxometalate retained the parent structure after being encapsulated by liposome and liposomal encapsulation increased the antitumoral activity of the polyoxometalate.