Nd0.67Sr0.33MnOy(Y＜3.0)中的自旋相关电致电阻效应

用固相反应法制备系列Nd0.67Sr0.33MnOy(y=3.00-2.80)多晶样品.样品输运性质表现出自旋相关电致电阻特征.对氧含量等于化学计量样品,在测量温度范围内电阻不随负载电流变化,I-V曲线符合线性欧姆定律.对氧含量低于化学计量样品,当高于某一特征温度时,电阻变化符合线性欧姆定律;但低于这一特征温度时,电阻大小与负载电流有关,I-V曲线偏离线性规律;在绝缘体-导体相转变点附近,样品电阻随负载电流增大而迅速减小,表现出巨大电致电阻效应.对于y=2.85样品,当电流从1μA增加到30μA时,电致电阻接近80%.这种自旋相关的电致电阻行为与氧含量和界面有很大关系.     

［Co(tren)(amino acidato-N,O)］X2·nH2O在溶液中的NMR研究

报道了配合物［Co(tren)(DL-phenylalaninato)］(ClO₄)₂ (Ⅰ)、Co(tren)(L-prolinato)］I₂·H₂O (Ⅱ)、［Co(tren) (L-valinato)］I₂·1/3H₂O (Ⅲ)、［Co(tren)(L-isoleucinato)］I₂ (Ⅳ)、［Co(tren) ( L-leucinato)］I₂ (Ⅴ) 在溶液中的NMR研究. 通过同核和异核二 维核磁共振实验归属了配合物的¹H和¹³C NMR ，发现在配合物的空间结构 中，四齿配体(tren)的3个螯合臂中有两个构象稳定，而另一个构象不稳定，这与晶体学数据吻合. 通过变温实验和溶剂效应实验，发现在配合物Ⅲ、Ⅳ、Ⅴ中存在分子内氢键，而在晶体结构中，所有配合物都存在分子间氢键. 配合物Ⅰ、Ⅱ在溶液中的行为需进一步的研究 .     

催化动力学光度法测定痕量锰--Mn(Ⅱ)-NTA-茜素紫3B-KIO4体系

在硼砂介质中 ,利用氨三乙酸活化 Mn( )催化 KIO4 氧化茜素紫 3B褪色的指示反应 ,建立了催化光度法测定痕量锰的新方法。方法的线性范围为 0 .0 30— 6 .0μg/ L ,检出限为 1.0× 10 -11g/ m L ,用于水样和茶叶中锰的测定 ,结果令人满意。     

含Eu3+离子的Na2O-K2 O-SiO2-Al2O3系统玻璃的制备及其变温发射光谱与结构特性

通过高温熔融法制备了含Eu^3 离子的Na2O-K2O-SiO2-Al2O3系统玻璃。在488nm波长光的激发下，系统地研究了上述玻璃从77K到700K温度范围的变温发光特征。发现总的荧光强度首先随温度的升高而大幅度升高，然后随温度的升高而减少，用声子辅助吸收与热激活过程及温度淬灭效应定性地解释了上述强度的变化，同时测量与分析了Eu^3 离子的晶格场参量。结果表明，Eu^3 离子与氧离子的距离随着温度升高而变短，而Eu^3 离子的配位数不随温度而变化。     

ICP-AES测定锰矿中二氧化硅含量

试样经氢氧化钠和过氧化钠混合熔剂碱熔,再用酸浸提,干过滤后定容.采用ICP-AES测定锰矿中二氧化硅含量.本法测定锰矿标样(冶金部标准样品505)中二氧化硅含量,其测定结果的相对标准偏差RSD为1.08%,测定平均值为33.93%(标样推荐值为33.58%).     

壳聚糖中ZnS：Mn纳米微晶的发光效率及时间分辨光谱

对制备的分散在壳聚糖中ＺｎＳ：Ｍｎ纳米微晶的红外吸收光谱，Ｘ射线衍射谱，激发和发射光谱，发光效率，时间分辨光谱进行了研究，讨论了发光性质变化的原因，实验表明，纳米微晶中Ｍｎ＾２＋的弛豫时间比体材料减少了约２个数量级，通过测量结果讨论了振子强度的变化。     

掺杂元素离子半径对LiMxMn2-xO4(M=Li,Na,T1)电化学性能的影响

以尿素为络合剂,氢氧化锂、醋酸锰等为原料通过水热反应获得颗粒均匀的尖晶石LiMxMn2-xO4(M=Li,Na,T1)前驱物,然后将前驱物在600℃～700℃间煅烧4h后获得最终产物.实验主要考察了掺杂元素的离子半径和M-O键离解能对产物LiMxMn2-xO4充放电过程中稳定性的影响,以及煅烧温度对材料形貌与结构的影响.结果表明掺杂元素的离子半径与被取代元素的离子半径越接近则掺杂后的材料越稳定,而M-O键离解能的影响则很小.实验发现LiNa0.02 Mn1.98O4的综合性能最佳,该样品在室温0.2C倍率的首次放电容量可以达到107 mAh·g-1,且不可逆容量衰减小,电池循环20次后容量只衰减了约2.8％.     

石墨探针技术／石墨炉原子吸收光谱测定人发中痕量锰

本文采用探针原子化技术对痕量锰进行了一系列条件试验，试验结果表明，石墨探针炉法具有灵敏度高，检出限低，重现性好，简便快速等特点，应用于人发中痕量锰的测定，结果满意。     

Finite size specimens with cracks of icosahedral AI-Pd-Mn quasicrystals

Icosahedral quasicrystals are the most important and thermodynamically stable in all about 200 kinds of quasicrystals currently observed. Beyond the scope of classical elasticity, apart from a phonon displacement field, there is a phason displacement field in the elasticity of the quasicrystal, which induces an important effect on the mechanical properties of the material and makes an analytical solution difficult to obtain. In this paper, a finite element algorithm for the static elasticity of icosahedral quasicrystals is developed by transforming the elastic boundary value problem of the icosahedral quasicrystals into an equivalent variational problem. Analytical and numerical solutions for an icosahedral A1-Pd-Mn quasicrystal cuboid subjected to a uniaxial tension with different phonon-phason coupling parameters are given to verify the validity of the numerical approach. A comparison between the analytical and numerical solutions of the specimen demonstrates the accuracy and efficiency of the present algorithm. Finally, in order to reveal the fracture behavior of the icosahedral A1-Pd-Mn quasicrystal, a cracked specimen with a finite size of matter is investigated, both with and without phonon-phason coupling. Meanwhile, the geometry factors are calculated, including the stress intensity factor and the crack opening displacement for the finite-size specimen. Computational results reveal the importance of pbonon-phason coupling effect on the icosahedral A1-Pd-Mn quasicrystal. Furthermore, the finite element procedure can be used to solve more complicated boundary value problems.     

Prototype of time digitizing system for BESⅢ endcap TOF upgrade

The prototype of a time digitizing system for the BESⅢ endcap TOF (ETOF) upgrade is introduced in this paper. The ETOF readout electronics has a distributed architecture. Hit signals from the multi-gap resistive plate chamber (MRPC) are signaled as LVDS by front-end electronics (FEE) and are then sent to the back-end time digitizing system via long shield differential twisted pair cables. The ETOF digitizing system consists of two VME crates, each of which contains modules for time digitization, clock, trigger, fast control, etc. The time digitizing module (TDIG) of this prototype can support up to 72 electrical channels for hit information measurement. The fast control (FCTL) module can operate in barrel or endcap mode. The barrel FCTL fans out fast control signals from the trigger system to the endcap FCTLs, merges data from the endcaps and then transfers to the trigger system. Without modifying the barrel TOF (BTOF) structure, this time digitizing architecture benefits from improved ETOF performance without degrading the BTOF performance. Lab experiments show that the time resolution of this digitizing system can be lower than 20 ps, and the data throughput to the DAQ can be about 92 Mbps. Beam experiments show that the total time resolution can be lower than 45 ps.