Synthesis and Crystal Structure of a Heteropentanuclear Yb(Ⅲ)-Cu (Ⅱ) Complex:[Yb_2Cu_3(O_2CCH_2CI)_(12)(H_2O)_8]·2H_2O

1INTRODUCTIONInterestinpolynuclearcomplexesisstimulatedbytherolestheyplayindifferentfields,e.g.heterogeneouscatalysis,bioinorganicchemistryandthedesignofmagneticmaterials.Since1985ill,considerableattentionshavebeengiventomolecularcomplexest'isimultaneouslycomprisingdandfmetalionsduetotheirspecialmagneticproperties.Coupledpolyr^uclearsystemscontaining3delementshavebeenextensivelyinvestigatedL,3,butonlyafew,derivedfromcarboxylatesL4--63,thatcontainbothtransitionandrare--earthmetalionshavebe…     

Tm3+/Yb3+ ∶LaF3纳米体系中掺杂Yb3+ 离子对Tm3+ 离子荧光发射的影响

为研究Yb³⁺离子浓度变化对Tm³⁺离子在蓝色波段荧光强度的影响,以NaF和La(NO₃)₃为原料,采用水热法制备了Tm³⁺和Yb³⁺共掺的Tm³⁺/ Yb³⁺∶LaF₃纳米颗粒.用X射线衍射对LaF₃纳米颗粒进行表征的结果显示,纳米晶体结构呈六方相.透射电镜的观测结果显示,纳米颗粒样品大小均匀、分散性良好.在波长为800 nm的激光激发下,观测到了上转换蓝光发射,其中包括波长为474 nm和479 nm的较强的荧光辐射(相应的跃迁为1G4→3H6)和波长位于450 nm的强度较弱的荧光发射(相应的跃迁为1D2→3F4).通过观测不同Yb³⁺离子浓度条件下共掺Tm³⁺/Yb³⁺∶LaF₃样品的荧光光谱,研究了Yb³⁺离子掺杂浓度对于Tm³⁺离子的荧光发射的影响,并探讨了产生这种现象的原因.研究结果显示,对于1G4→3H6跃迁产生的荧光发射(474 nm),当Yb³⁺离子浓度增大时,反向能量传递速率的增加导致了荧光强度的增大.然而,当Yb³⁺离子浓度增大到一定程度时,Yb³⁺离子激发态能级寿命的减少将引发荧光强度的下降.相比较而言,Yb³⁺离子的浓度的变化对于1D2→3F4跃迁产生的位于450 nm处荧光强度的影响较弱.     

加拿大一枝黄花总酚超声提取工艺

利用超声提取的方法,通过单因素和正交实验分析了溶液浓度、超声时间、料液比、提取次数4个主要因素对总酚提取率的影响。确立了加拿大一枝黄花总酚的最佳提取工艺条件为:60%甲醇、超声50min、料液比1∶20、提取3次。在此条件下,总酚的提取率为44.61mg/g。     

平面镜演示实验仪器的研制和成像分析

阐述了平面镜演示实验仪器的设计与制作、使用方法及观察到的实验现象,并从光学成像的角度分析和探讨了相应的物理原理.     

Thermal analysis and expected performance of the low energy instrument on board the HXMT satellite

The Low Energy X-ray Instrument (LE) of the Hard X-ray Modulation Telescope (HXMT) uses the Swept Charge Device (SCD) to detect the X-rays in 1-15 keV. The performance of SCD is vulnerable to temperature. We analyzed the thermal condition of LE at different satellite working attitudes with the Finite Element Method (FEM). It is shown that the angle between the sunlight and the normal line of the barrier should be less them 26°, to keep the SCD detectors working in the required temperature range, i.e. -40 ℃ to -80 ℃. We find that the performance of LE is very stable in this temperature range, with a typical energy resolution of 160 eV at 5.9 keV.     

微型平像场近红外光谱仪的消杂散光设计

设计和研制了结构紧凑、杂散光低的微型平像场近红外光谱仪。在分光系统设计中不采用附加杂散光遮挡装置的常规方法,而是在准直物镜前设置一块直径为8．5mm的平面反射镜,通过调节平面反射镜改变入射光束的空间角,使光束全部被准直镜接收,不再产生旁光,从而有效地消除系统内的杂散光,使仪器整体杂散光水平降低了1．13％。另外,该光谱仪选择线阵CCD作为探测器件,不再设置冷却系统也避免了平面光栅带有扫描旋转机构。由于使用CCD作探测器和新的消杂散光设计方法,该光谱仪实现了微型化。     

污染数据半参数回归模型中估计的相合性

利用最小二乘估计方法和权函数法给出了半参数模型Y=βX g(T) ε在某种污染方式下,,βg和污染系数的估计,并在适当条件下证明了它们具有相合性.     

Observation of B(s)0-->K+ K- and measurements of branching fractions of charmless two-body decays of B0 and B(s)0 mesons in pp collisions at square root of s = 1.96 TeV

We search for decays of the type B(s)0-->h+ h'- (where h,h' = K or pi) in 180 pb(-1) of pp collisions collected at the Tevatron by the upgraded Collider Detector at Fermilab. We report the first observation of the new mode B(s)0-->K+ K- with a yield of 236+/-32 events, corresponding to (fs/fd) x B(B(s)0-->K+ K-)/B(B0-->K+ pi-) = 0.46+/-0.08stat+/-0.07syst, where fs/fd is the ratio of production fractions of B(s)0 and B0. We find results in agreement with world averages for the B0 modes, and set the following new limits at 90% C.L.: B(B(s)0-->K- pi+) < 5.6 x 10(-6) and B(B(s)0-->pi+ pi-) < 1.7 x 10(-6).     

Structure-antibacterial activity relationship of secondary metabolites from Ajuga pseudoiva Rob. leaves

A selection of steroids, glycerides, clerodane diterpenoids, and a beta-hydroxy fatty acid methyl ester, all previously isolated from Ajuga pseudoiva leaves, were tested for their antibacterial activity toward three Gram- rods and one Gram+ coccus using the dilution method; MIC values were determined. The results suggested some importance for a free beta-hydroxy group in the fatty acid ester and also in the glycerides and clerodane derivatives; the absolute configurations of the latter, notably at C2, had little influence on activity.