钯在乙醇水溶液中与钌、银、铜和铅的析相绿色萃取分离

在硫酸铵存在下,乙醇水溶液能够分为醇/水两相,在分相过程中,Pd²⁺与KBr和C₂H₅OH₂⁺生成的[PdBr₄^2-][C2HsOH-2⁺]₂三元缔合物能被乙醇相萃取,使Pd²⁺与Ru²⁺、Ag⁺、Cu²⁺和Pb²⁺完全分离。该法在微量钯的分离和富集分析中有一定的实用价值。     

交换纤维柱分离ICP-AES测定高纯氧化镱中La、Nd、Eu和Gd

以强酸型离子交换纤维柱分离富集高纯Yb₂O₃中La,Nd,Eu和Gd等痕量杂质元素,并用Optima 5300 DV ICP-AES测定分离富集后的这4种元素。供试纤维对Yb的动态吸附容量为134 mg·g-1,4.0 g纤维柱的分离条件为：pH 3.00的试液以1.0 mL·min-1流速上柱后,分离柱先以流速为1.5 mL·min-1的pH 3.00 HNO₃溶液80 mL预淋洗,再以同样流速pH 5.00的0.01 mol·L-1 EDTA铵溶液淋洗。结果表明：10 mg Yb与各为0.100 μg的La,Nd,Eu和Gd能达到基线分离;分离含100 mg Yb的试液后,在杂质富集液中Yb的残留浓度仅为0.017 1 μg·mL-1。 研究显示,当待测试液中Yb₂O₃的浓度小于100 μg·mL-1(如Yb 87.8 μg·mL-1)时,它对测定La,Nd,Eu和Gd等杂质元素的基体干扰可以忽略不计。富集倍数分别为La₂O₃ 3.68×105,Nd₂O₃ 4.20×105,Eu₂O₃ 3.82×105,Gd₂O₃ 4.01×105。方法检出限分别为La₂O₃ 0.005 0 pg·mL-1,Nd₂O₃ 0.014 pg·mL-1,Eu₂O₃ 0.001 8 pg·mL-1,Gd₂O₃ 0.008 2 pg·mL-1。本方法已用于99.99% Yb₂O₃样品中4种稀土杂质的测定,标准加入的平均回收率分别为La₂O₃ 94.2%,Nd₂O₃ 107%,Eu₂O₃ 97.8%,Gd₂O₃ 102%,RSD (%, n=5)分别为La₂O₃ 6.2,Nd₂O₃ 5.9,Eu₂O₃ 7.3,Gd₂O₃ 2.5,校正曲线不需进行Yb的基体匹配,分析周期为4 h。     

铌酸锶钠锂单晶电光、热电、介电和压电性能

文本研究了用提拉法生长的铌酸锶钠锂(Sr₄NaLiNb₁₀O₃₀)晶体的电光、热电、介电和压电性能。其半波电压与温度的关系与晶体中锂含量密切相关。测得其室温下的热电系数与Ba～0.5的Sr_1-xBa_xNb₂O₆晶体相当,～7×10^-8C/cm²·K。已极化的晶体几乎检测不到退极化现象。将其作成热电器件,其探测度D^*不小于1.7×10⁷Hz^1/2·cm/W。文中还描述了其介电和某些压电性能。 关键词：     

水溶液中稀土离子与甘氨酸、丝氨酸、天冬氨酸作用的13C NMR研究

测定了酸性水溶液中甘氨酸、丝氨酸和天冬氨酸稀土络合物(Ln=La、Pr、Nd、Eu、Tb、Dy、Ho、Er、Tm和Yb)的¹³C诱导位移。对位移试剂的分析指出,三种氨基酸通过α-羧基以双齿形式配位于稀土,配位键长为0.23nm~0.25nm,天冬氨酸的γ-羧基也是配位基团。由本文与文献中已报道的各种氨基酸稀土络合物的¹³C诱导位移的系统分析表明,配体¹³C超精细偶合常数A值和结构因子G值有如下规律:(1)│A(C₀)│<│A(C_α)│;A(C₀)为正,A(C_α)为负;(2)│G(C₀)│>│G(C_α)│;配体碳核的G均为负值。     

Tb3+,Eu3+单掺杂、双掺杂SrSiO3的合成、结构表征与发光性能

采用液相沉淀法合成了铽单掺杂,铕单掺杂,铽、铕双掺杂的硅酸锶发光材料。其结构经X-射线衍射表征。研究了合成样品的激发、发光光谱。研究结果表明:在254nm波长紫外光激发下,SrSiO₃:0.04Eu³⁺的发光光谱中出现4个Eu³⁺的发光峰,分别为Eu³⁺的⁵D₀→⁷F₁（588、590nm）、⁵D₀→F₂（609nm）、⁵D₀→⁷F₃（626nm）、⁵D₀→⁴F₄（651nm）跃迁峰;SrSiO₃:0.04Tb³⁺的发光光谱中出现4个Tb³⁺的发光峰,分别为Tb³⁺的⁵D4→^F₆（488nm）、⁵D₄→⁷F₅（541、548nm）、⁵D₄→⁷F₄（584nm）跃迁峰;SrSiO₃:0.04Tb³⁺,0.04Eu³⁺发光体系中,Tb³⁺的共掺杂显著增强了Eu³⁺的特征发射,存在Tb³⁺→Eu³⁺的能量传递现象,结果表明有Eu³⁺和Tb³⁺两个发光中心。     

硅、锗中氧的低温红外吸收

在6—300K下,利用红外傅里叶光谱仪研究了400—4000cm^-1间的硅、锗中氧的红外吸收。采用高分辨条件时,分辨率可达0.5cm^-1。研究了在低温下利用硅的1106cm^-1吸收峰和锗的855cm^-1吸收峰探测硅和锗氧含量的探测限和误差。若样品厚度为2cm,估计在20K下,硅中氧含量探测限～9.6×10¹⁴氧原子·cm^-3,锗中氧含量探测限～3.0×10¹⁴氧原子·cm^-3。同时,对不同生长条件下直拉锗单晶的氧含量进行了研究,并与用锂沉淀法所求得的锗中氧含量加以比较。对不同氧含量的硅样品的1106cm^-1吸收峰在6—300K的变化进行了观察和讨论。 关键词：     

锂、硼、硅酸盐玻璃体系的11B核磁共振研究

利用¹¹B的核磁共振谱研究了锂、硼、硅酸盐(Li₂O·B₂O₃·SiO₂)三元玻璃体系,测量并分析了BO₄单元与对称和非对称的BO₃单元的比例。分析结果表明,三元体系的结构单元亦可适用于锂、硼玻璃的二元体系的FDB模型说明,其差异在于前者中的Li₂O由B₂O₃与SiO₂按比例分享。     

对氨基马尿酸铽二元、三元配合物的合成、表征及荧光光谱研究

在乙醇溶液中以邻菲咯啉(phen)、2,2’-联吡啶(bipy)和对氨基马尿酸(PAH,HL)为配体与铽离子(Tb(Ⅲ))合成了二元和三元稀土配合物。通过元素分析、差热-热重分析、紫外光谱、红外光谱分析,确定了配合物的组成为TbL₃(1)、TbL₃·phen·H₂O(2)和TbL₃·bipy·H₂O(3),并讨论了配合物1～3的谱学性质和荧光性能。推测出羧基中的氧原子以桥式双齿的形式与稀土离子配位。由红外光谱和热分析测试确定的配合物1及配合物2中的水分子未参与配位。研究表明,铽配合物在489,583和621 nm处出现发射峰,它们分别归属于5D₄→7F₆,5D₄→7F₅,5D₄→7F₄和5D₄→7F₃的跃迁。其中544 nm处5D₄→7F₅跃迁的强度最强,配体的共平面性和共轭性越大,配合物的荧光性能越高,三元配合物TbL₃·phen·H₂O和TbL₃·bipy·H₂O的荧光强度优于二元配合物TbL₃的荧光强度。     

Charmed Deuteron

Possible existence of bound states of a charmed baryon, Λ _c , Σ _c , Σ* _c with a nucleon, N, as well as two charmed baryons, Λ _c Λ _c , etc., are examined in the meson exchange potential approach. The heavy quark spin symmetry induces a strong tensor coupling between Λ _c N, Σ _c N and Σ* _c N states, which causes a bound state of Λ _c N (J = 0⁺ and 1⁺) states. Such a bound state is also seen in the spin-singlet Λ _c Λ _c channel, which resembles the H dibaryon in the strange sector.     

锌的X射线热漫散衍射及弹性系数

提出使用逐步逼近方法进行X射线热漫散衍射强度的水平与垂直发散修正。从测量的热漫散衍射强度经过各种修正之后,得到锌的弹性系数与超声方法得到的结果相符,分别为(以10¹²达因/厘米²为单位):c₁₁=1.6₉,c₁₂=0.39₄,c₁₃=0.54₉,c₃₃=0.68₂,c₄₄=0.42₉,c₆₆=(1/2c₁₁-1/2c₁₂=0.64₈。     

GaAs及其它半导体欧姆接触模型

n型GaAs欧姆接触的比接触电阻ρ_c与有源层浓度N_D有反比关系,这已为很多实验事实所证明。文献中对这一现象有各种解释。本文对文献中的各种解释模型进行了分析,指出不足之处。提出ρ_c应由两部分ρ_(c1)和ρ_(c2)组成。ρ_(c1)是合金与其下在合金化后形成的高掺杂层间的比接触电阻。此外,在这高掺杂层与原来有源层间有 关键词：     

Lattice softening in K2Pt(CN)4Br0.3·3H2O

The temperature dependences of the elastic constants, c₁₁, c₃₃, c₄₄, and c₆₆, in KCP are described. In the temperature range 10–100 K softening is observed in c₄₄, while c₆₆ decreases almost linearly with decreasing temperature. These results indicate the presence of a new critical region.     

The pressure dependence of the superconducting transition temperature of LaT4P12(T = Fe,Ru, Os)

The superconducting transition temperature, T_c, of the LaT₄P₁₂ compounds with T = Fe, Ru, or Os has been measured under hydrostatic pressure P up to 1.8 GPa. The T = Fe compound exhibits a substantial increase of T_c from T_c (P = 0) = 4.1 K at a rate (dT_c/dP)_P=0= +7.2 x 10^-1 K/GPa. In contrast, the Ru and Os compounds exhibit only weak decreases of T_c from T_c (P = 0) = 7.2 K and 1.8 K with (dT_c/dP)_P=0= -1.6 x 10^-1 K/GPa and -9.5 x 10^-2 K/GPa, respectively. An analysis of this strikingly divergent behavior of T_c(P) in terms of the structural characteristics of the RT₄X₁₂ class of compounds where R = rare earth element, T = Fe, Ru, or Os, and X = P, As, or Sb suggests that T_c(P) for these materials consists of two competing contributions: a depression of T_c due to the compression of the lattice (i.e., decrease in volume), and an enhancement of T_c due to the effect of pressure on La itself.     

Effects of neutron irradiation on superconducting properties of orthorhombic Y–Ba–Cu oxides

Abstract

We have studied the effects of fast neutron (E>0.1 MeV) irradiation at reactor (～ 360 K) and low (～ 20 K) temperatures on the superconducting properties of polycrystalline orthorhombic YBa₂Cu₃O_7?y . Measurements were made on the superconducting critical temperature T_c , critical current J_c , Meissner effect and magnetic field dependence of J_c . The T_c drops by an irradiation at reactor temperature and J_c increases with increasing fluence. On the other hand with the irradiation at low temperature, T_c rises and J_c increases. Results of observation of Meissner effect and the magnetic field dependence of J_c are consistent with the behavior of T_c and J_c .     

Exact quantum partition function of the BCS model

The exact calculation of the reduced BCS model quantum partition function (QPF) in the thermodynamic limit is carried out by the path integration method. The expression for the QPF and the phase transition temperatureT _c in the regular phase coincide with the results of Bogolyubov. In the nonregular phase a temperature singularity appears in the expression for the QPF: the QPF diverges in the region of temperaturesT _c which are smaller than some critical temperatureT _c ^* , and it turns out that in all casesT _c ^* > T _c and the differenceT _c ^* –T _c is not small. The interpretation of the temperatureT _c ^* is given.     

c-axis penetration depth in Bi2Sr2CaCu2O8+δ single crystals measured by ac-susceptibility and cavity perturbation technique

The c-axis penetration depth Δλ_c in Bi₂Sr₂CaCu₂O_8+δ (BSCCO) single crystals as a function of temperature has been determined using two techniques, namely, measurements of the ac-susceptibility at a frequency of 100 kHz and the surface impedance at 9.4 GHz. Both techniques yield an almost linear function Δλ_c(T)∝T in the temperature range T<0.5T _c. Electrodynamic analysis of the impedance anisotropy has allowed us to estimate λ_c(0)≈50 µm in BSCCO crystals overdoped with oxygen (T _c≈84 K) and λ_c(0)≈150 µm at the optimal doping level (T _c≈90 K).     

Experimental review of e~+e~-→ππh_c

We review the recent BESIII measurement of e~+e~-→ππh_c in which its line shape is studied between the center-of-mass energies of 3.9 to 4.42 Ge V and an iso-vector charmonium-like state Z_c(4020) is observed in the invariant mass of πhc at the BESIII experiment. The charged Z_c(4020)~± is the second observed Z_c state following Z_c(3900), while the Z_c(4020)~0 is the first observed neutral Z_c state. The line shape of σ(e~+e~-→ππh_c) is also reanalyzed in view of searching for the Y state and the existence of the Y(4220) state is confirmed and compared with the previous work of the BESIII experiment.     

含Sb的Bi系超导体的研究

Bi-Sr-Ca-Cu-O系中掺入适量的Sb,其高温相(110K相)含量明显多于不掺Sb样品。Sb具有加速高温相形成的作用。对于各义组分为Bi_2-xSb_xSr₂Ca_2.5Cu_3.7O_y的样品,x=0.1最有利于高温相的形成。用液氮中淬火后低温回火的方法,发现在865℃烧结时样品中首先形成的是低温相(80K相),然后再逐渐转变为高温相。T_c值随烧结时间的延 关键词：