基于{PMo_(12)O_(40)(VO)_(0.5)}的Cu(Ⅰ)配合物的合成及荧光性质研究

利用磷钼十二酸、偏钒酸铵、CuCl_2·2H_2O和3,3′,5,5′-四甲基-4,4′-联邻二氮杂茂(H_2X)在水热条件下反应,合成出了1个新的多酸基杂化化合物Cu_4(H_2X)_4[(PMo_(12)O_(40)(VO)_(0.5))].通过X射线单晶衍射、红外光谱和热重分析等测试手段对该化合物进行了结构表征.单晶结构解析表明该化合物为2D层状化合物,属于单斜晶系,C2/c空间群,晶胞参数a=2.637 6(5)nm,b=1.542 2(5)nm,c=2.057 0(5)nm,α=90.000(5)°,β=112.677(5)°,γ=90.000(5)°,V=7.720(3)nm~3,Z=4,R_1=0.061 5,wR_2=0.164 6.     

Br~-掺杂Bi_2WO_6的水热法合成及其可见光催化性能

以Bi(NO_3)_3·5H_2O和Na_2WO_4·2H_2O为主要原料,采用水热法合成了纯相Bi_2WO_6,并对其进行非金属离子Br-掺杂改性。采用XRD、SEM、TEM、XPS、Raman、PL和DRS研究了Br~-掺杂对Bi_2WO_6的物相结构、形貌和可见光催化性能的影响。结果表明,Br-掺杂可有效提高Bi_2WO_6的可见光催化性能,当掺杂量(物质的量百分数)为8%时,溴掺杂Bi_2WO_6的光催化性能最好,可见光照射40 min后,可降解96.73%的罗丹明-B,与未掺杂Bi_2WO_6相比,其降解率提高了36.32%。     

重金属铊在环境介质中的分布及其迁移行为

铊是剧毒重金属元素,它在自然界中是典型的稀有分散金属。环境介质中铊的自然本底值较低,但随着铊矿床的开发和铊资源的广泛应用,岩矿石中的铊在自然力或人为作用下向环境介质中迁移。综述了铊在岩（矿）石、土壤、水体、动植物和人体中的分布,以及在上述环境介质及大气中的迁移行为。研究表明,人类活动是导致环境介质中铊含量增加的主要原因。铊在环境介质中的迁移是反复循环的复杂过程,通过风化、溶解、淋滤、吸收、沉降、固结等方式在环境介质中循环往复,从而危害环境生态和人体健康。铊污染应引起人们的普遍重视。     

促红细胞生成素B螺旋表面肽的代谢稳定性结构修饰：设计、合成及其提高的肾保护作用

肾脏缺血缺氧以及再灌注过程都将导致肾小管上皮细胞凋亡,使肾功能严重受损.肾脏的缺血再灌注损伤是移植肾功能延迟恢复的主要原因并能诱导急慢性排斥,影响肾存活率.近年来发现,衍生于促红细胞生成素（EPO）的B螺旋亚基亲水表面序列的肽链（HBSP）,对肾脏缺血再灌注损伤具有显著的保护作用,但其在体内极短的半衰期（约2min）极大地限制了它的临床应用.因此,本研究采用构象约束、全D-构型氨基酸替换和N-端封闭策略,设计了3种类型的EPOB螺旋表面肽衍生物,旨在提高其代谢稳定性环肽的设计采用了对氧化还原稳定的硫醚键和相对刚性的亚砜键两种环合方式.在多肽的合成上,采用微波辅助多肽自动合成和手工合成两种模式有机结合;优化了硫醚环合工艺,应用微波加热进行硫醚环肽的合成,大大提高了产率和效率;利用圆二色（CD）谱确定了亚砜环肽的相对构型.活性实验表明,相对于线性母肽HBSP,本文设计合成的代谢稳定衍生肽对大/小鼠肾脏缺血再灌注损伤均有显著提高的保护作用,且硫醚和R-构型亚砜环肽的肾脏保护活性强于S-构型亚砜环肽.而且,环化确实提高了功能肽的血浆稳定性.因此,本文合成的硫醚环肽一周一次注射剂量等效于线性肽HBSP一日三次剂量对小鼠肾损伤的保护作用.     

MgF2对Mn4+掺杂锗酸盐红色荧光粉发光的影响

3.5MgO·0.5MgF₂·GeO₂∶Mn⁴⁺作为优异热稳定性和良好发光性能的红色荧光粉而被市场应用,然而,该粉体中MgF₂的作用影响机理尚不明晰,阻碍其性能进一步优化和发展。采用高温固相法制备了系列Mn⁴⁺激活的锗酸盐荧光粉,通过对比加入MgF₂、H₃BO₃(助熔剂),研究了该粉体的结构、形貌、发光性能等变化规律,阐明了MgF₂的发光影响作用。研究表明,加入MgF₂、H₃BO₃和不加任何助熔剂时的样品,其最佳烧结温度分别为1 150、1 250和1 350 ℃,上述温度下发光强度均为最佳值,其中加入MgF₂、H₃BO₃的样品在最佳温度处生成了纯相。MgF₂的添加,一方面同H₃BO₃一样作为助熔剂对生成纯相、提高样品结晶度起了积极的作用;另一方面,通过研究分析,确认F^-离子成功掺杂进入晶格,促使样品生成的晶体结构为Mg₁₄Ge₅(O,F)₂₄。加入MgF₂、H₃BO₃在最佳烧结温度的样品的荧光寿命分别为0.93和0.75 ms。     

基于四甲基取代胍环的四核稀土镝簇合物的慢磁弛豫

报道了2个基于四甲基取代胍环的三明治型四核稀土簇合物, [Ln₄(μ₃-OH)₄(μ₂-OH)₂(H₂O)₄(NO₃)₂(TMeQ[6])₂]·(NO₃)₄·26H₂O(Ln=Dy, 1; Ln=Tb, 2)。晶体结构分析显示2个簇合物包含2个四甲基取代胍环夹心的四核稀土立方烷结构, [Ln₄(μ₃-OH)₄]⁸⁺。磁性研究显示化合物1显示了慢磁弛豫行为。由于胍环配体可以有效的传递能量给稀土铽离子, 化合物2具有较好的发光性能。     

Br-掺杂Bi2WO6的水热法合成及其可见光催化性能

以Bi（NO₃）₃·5H₂O和Na₂WO₄·2H₂O为主要原料,采用水热法合成了纯相Bi₂WO₆,并对其进行非金属离子Br^-掺杂改性。采用XRD、SEM、TEM、XPS、Raman、PL和DRS研究了Br^-掺杂对Bi₂WO₆的物相结构、形貌和可见光催化性能的影响。结果表明,Br^-掺杂可有效提高Bi₂WO₆的可见光催化性能,当掺杂量（物质的量百分数）为8%时,溴掺杂Bi₂WO₆的光催化性能最好,可见光照射40 min后,可降解96.73%的罗丹明-B,与未掺杂Bi₂WO₆相比,其降解率提高了36.32%。     

Conceptual design of an intense positron source based on an LIA

Accelerator based positron sources are widely used due to their high intensity. Most of these accelerators are RF accelerators. An LIA (linear induction accelerator) is a kind of high current pulsed accelerator used for radiography. A conceptual design of an intense pulsed positron source based on an LIA is presented in the paper. One advantage of an LIA is its pulsed power being higher than conventional accelerators, which means a higher amount of primary electrons for positron generations per pulse. Another advantage of an LIA is that it is very suitable to decelerate the positron bunch generated by bremsstrahlung pair process due to its ability to adjustably shape the voltage pulse. By implementing LIA cavities to decelerate the positron bunch before it is moderated, the positron yield could be greatly increased. These features may make the LIA based positron source become a high intensity pulsed positron source.     

A design study of a magnifying magnetic lens for proton radiography

Magnifying magnetic lenses can be used in high-energy proton microscopes. The -I lens suggested by Zumbro is analyzed in this paper, and a new type of magnetic lens called a lengthened lens is introduced. Theoretical analysis shows that the lengthened lens can form a magnifying lens, and at the same time the main advantages of a Zumbro lens are inherited. Using the My-BOC beam dynamics code, an example of the design is shown. The results show that the method of designing magnifying magnetic lenses is effective.     

Formation of multiple dark photovoltaic spatial solitons

We theoretically study the formation of multiple dark photovoltaic soliton splitting in the quasi-steady-state and steady-state regimes under open-circuit conditions. We find that the initial width of the dark notch at the entrance face of the crystal is a key parameter for generating an even (or odd) number sequence of dark coherent photovoltaic solitons. If the initial width of the dark notch is small, only a fundamental soliton or Y-junction soliton pair is generated. As the initial width of the dark notch is increased, the dark notch tends to split into an odd (or even) number of multiple dark photovoltaic solitons, which realizes a progressive transition from a low-order soliton to a sequence of higher-order solitons. The soliton pairs far away from the centre have bigger width and less visibility. In addition, when the distance from the centre of the dark notch increases, the separations between adjacent dark stripes become slightly smaller.