邻苯二甲酸钙的热分解反应研究

用热重和示差扫描量热分析法研究了-水合邻苯二甲酸钙的热分解过程。其热分解过程分为三个阶段: 在160~260℃脱水生成无水盐; 在460~780℃分解生成CaCO~3.C; 在780~900℃生成CaO和CO。用粉未X射线衍射、红外光谱和色-质联用分析法表征了各阶段热分解产物的组成和结构。讨论了热分解产物的自由基反应机理。     

Enhancement of electron–ion recombination rates at low energy range in the heavy ion storage ring CSRm

Recombination of Ar¹⁴⁺, Ar¹⁵⁺, Ca¹⁶⁺, and Ni¹⁹⁺ ions with electrons has been investigated at low energy range based on the merged-beam method at the main cooler storage ring CSRm in the Institute of Modern Physics, Lanzhou,China. For each ion, the absolute recombination rate coefficients have been measured with electron–ion collision energies from 0 meV to 1000 meV which include the radiative recombination(RR) and also dielectronic recombination(DR)processes. In order to interpret the measured results, RR cross sections were obtained from a modified version of the semiclassical Bethe and Salpeter formula for hydrogenic ions. DR cross sections were calculated by a relativistic configuration interaction method using the flexible atomic code(FAC) and AUTOSTRUCTURE code in this energy range. The calculated RR + DR rate coefficients show a good agreement with the measured value at the collision energy above 100 meV.However, large discrepancies have been found at low energy range especially below 10 meV, and the experimental results show a strong enhancement relative to the theoretical RR rate coefficients. For the electron–ion collision energy below 1 meV, it was found that the experimentally observed recombination rates are higher than the theoretically predicted and fitted rates by a factor of 1.5 to 3.9. The strong dependence of RR rate coefficient enhancement on the charge state of the ions has been found with the scaling rule of q^3.0, reproducing the low-energy recombination enhancement effects found in other previous experiments.     

南极磷虾油中总砷含量及砷形态分析

南极磷虾油富含Omega-3磷脂而具有强大的保健功能,但由于其砷含量较高,在保健品领域的应用受到一定限制.由于南极磷虾油中含有大量的磷脂质,采用常规的提取方法分析难以对其砷形态进行准确定量分析.本研究采用高效液相色谱-电感耦合等离子体质谱((HPLC-ICP-MS)联用技术建立了针对砷甜菜碱(AsB)、二甲基砷酸(DMA)、一甲基砷酸(MMA)、三价砷As(Ⅲ)、五价砷As(Ⅴ)5种砷形态的分析方法.采用C18固相萃取进行样品脱脂前处理,采用阴离子交换色谱IonPac AS9-H阴离子分析柱(250 mm×4 mm),流动相采用38 mmol/L Na2SO4+15 mmol/L乙酸钠;流速0.6 mL/min,流速1 mL/min,进行5种形态砷化合物的分析.结果表明,5种砷化合物的线性范围为0.5～500 μg/L,相关系数R＞0.9993.检出限(LOD)为0.1 ～0.2 μg/L,定量限(LOQ)为1.5 ～2.6 μg/L,RSD＜5％.加标回收率为88.9％ ～ 106.3％.样品的测定结果显示,南极磷虾油中砷形态的主要存在形式为无毒的砷甜菜碱,因此可以安全地应用于食品及保健品.     

制备铋靶的脉冲电镀工艺

 采用脉冲电镀工艺,以直径为1 mm的铜丝为芯轴,在无氰镀液体系中,制备出惯性约束聚变实验用铋靶所需的金属铋镀层。通过正交试验得到的最佳脉冲工艺条件为：电流密度5 A/cm²,频率600 Hz,占空比1∶6,温度20 ℃。利用扫描探针显微镜和扫描电子显微镜分别对铋镀层表面形貌进行分析,同时利用X射线衍射对铋镀层物相成分进行分析。表征结果表明：所得铋镀层表面细致均匀,孔隙率低,平整性好,无裂纹。     

磁控溅射制备的铜钒氧化物薄膜及其电化学性能

采用射频磁控溅射技术在硅基底上分别制备了无掺杂和掺杂Cu的氧化钒薄膜. X射线衍射(XRD)分析和扫描电子显微镜(SEM)观察表明, 无掺杂的薄膜为多晶V2O5, 掺杂Cu的薄膜为非晶态. X射线光电子能谱(XPS)分析结果表明, 掺杂Cu的薄膜为铜钒氧化物膜, 其中Cu离子表现为+2价, V离子为+4与+5价的混合价态. 随着Cu掺杂量的增大, +4价V的含量增加. 电化学测试结果表明, V2O5薄膜在掺杂Cu以后其放电容量有显著的提高, 其中Cu2.1VO4.4薄膜在100次循环后容量还保持为83.4 μA·h·cm-2·μm-1, 表现出较高的放电容量和较好的循环性能.     

掺杂Eu3+的Na24As2Mo22O83的合成及其发光特性

本文在固相合成掺杂稀土离子的单钨酸盐,混合碱土金属钨酸盐^[1-3]等体系的的系统研究基础上,采用固相反应法合成掺杂Eu^3 离子的Na24As2Mo22O83荧光体结晶粉末,并经元素分析,IR和X射线粉末衍射等分析手段确定了它的结构,探讨了Eu^3 离子在Na24As2Mo22O83中的发光和能量传递机理。     

钼在钨酸钙荧光体中的能量传递研究

合成一系列掺杂钼的乌酸钙荧光体，通过测定系列荧光体的发射光谱系统地研究了其发光特性，探讨了钼在钨酸钙荧光体中的能量传递机理。     

IH型漂移管直线加速器的束流动力学研究（英文）

为了提高兰州重离子加速器冷却储存环（HIRFL-CSR）的运行效率、改善加速器输出束流品质,并实现几个加速装置分时供束,提高整个重离子加速装置的利用率,特为（HIRFL-CSR）增建一台新的注入器--CSRLINAC。在108.48 MHz的RFQ之后的CSR-LINAC主加速段,主要由一台108.48 MHz和两台216.96 MHz的IH型漂移管直线加速器组成,用于加速荷质比为1/8.5~1/3之间的重离子,其最大的束流流强为3 mA,并将粒子从0.3 MeV/u加速到3.71 MeV/u。运用KONUS动力学原理,在满足设计指标的情况下,首先利用TraceWin程序进行中能束线MEBT设计,后针对高频腔体设计和束流匹配的基本参数的系列讨论,特别是对CSR-LINAC的中能束流匹配线、参数选择和IH型KONUS结构的漂移管直线加速器进行设计模拟优化。最终得出,在保证腔体设计指标和95.3%的传输效率的情况下,该紧凑型直线加速结构经过三个腔体的加速后,束流的纵向归一化均方根发射度增长仅有25%;同时发现,当流强达到3 mA时,存在空间电荷效应,导致其纵向相宽增长约25%,最大横向包络也存在16.5%的涨落。In order to improve the operation efficiency of the Cooling Storage Ring of Heavy Ion Research Facility in Lanzhou (HIRFL-CSR), a heavy ion linac (linear accelerator) was proposed and designed as a new injector for HIRFL-CSR. Following the 108.48 MHz Radio-Frequency Quadrupole (RFQ), three tanks in total with Interdigital H-mode drift tube linac (IH-DTL) structure are installed to boost the beam energy from 0.3 to 3.71 MeV/u, and the beam current of ions with charge-to-mass ratio from 1/8.5 to 1/3 can reach to 3 mA. The first tank operatesat the same frequency as the RFQ, and the rest two operate at 216.96 MHz. The “Combined Zero-Degree Synchronous Particle Structure” (KONUS) beam dynamics was used in the beam dynamics design. The overview of the physics design on the main accelerating components, including RF design and beam dynamics design are introduced in this paper. The optimized structure design, fabrication status and simulation results are presented in this contribution. It shows that under the condition of assurance of 95.3% transmission efficiency, the normalized rms emittance is about 25%. When the beam current is up to 3 mA, owing to the space charge effect, the increase of longitudinal phase spread and transverse envelope are about 25% and 16.3%, respectively.     

以联吡啶二羧酸及邻菲咯啉衍生物为配体的两种锌(Ⅱ)配合物的水热合成及晶体结构

在水热条件下合成了两种配合物[Zn(bpdc)(pyip)2].3H2O(1)和[Zn(pip)2(Hpip)].3H2O(2)(H2bpdc=2,2′-联吡啶-3,3′-二羧酸,pyip=2-(3-吡啶基)-1H-咪唑并[4,5-f][1,10]邻菲咯啉,Hpip=2-苯基-1H-咪唑并[4,5-f][1,10]邻菲咯啉),并利用红外和X射线单晶衍射对其结构进行了表征。配合物1属单斜晶系,P21/c空间群,晶胞参数a=1.656 9(5)nm,b=1.3614(4)nm,c=1.863 7(6)nm,β=93.128(6)°,V=4.198(2)nm3,Z=4,ZnC48H34N12O7,Mr=955.99,Dc=1.513 g.cm-3,μ(Mo Kα)=0.657 mm-1,F(000)=1 968,GOOF=1.008,R=0.057 7,wR=0.107 5,其中4 622个可观测衍生点(I>2σ(I))。配合物2属单斜晶系,P21/c空间群,晶胞参数a=1.797 7(4)nm,b=1.527 0(3)nm,c=1.767 6(4)nm,β=102.84(3)°,V=4.730 9(19)nm3,Z=4,ZnC57H40N12O3,Mr=1 006.36,Dc=1.410 g.cm-3,μ(Mo Kα)=0.581mm-1,F(000)=2 072,GOOF=1.134,R=0.089 5,wR=0.208 4,其中6 558个可观测衍射点(I>2σ(I))。结构分析表明配合物1和2均为零维结构,氢键和π-π相互作用在加固配合物的结构中起到重要作用。此外,对化合物的热稳定性和荧光性质也进行了研究。     

两维有限深势阱中BEC的稳定性分析

研究两维轴对称有限深势阱中BEC的稳定性,利用变分法分别讨论了系统的基态和激发态特性。研究表明系统存在塌缩态、束缚态和扩散态三种状态,并计算出系统状态发生变化的耦合常数的两个临界值,发现势阱的形状与系统的稳定性紧密相关。同时在激发态下进一步讨论了原子间相互作用发生周期性调制的BEC的动力学特性,分析发现有限深势阱中BEC的塌缩可以通过周期性调制散射长度来控制。本文最后讨论了涡旋态下BEC的稳定性,发现系统的塌缩点由于涡旋态的存在而降低。