Structural and superconducting properties in Y0.6Gd0.4Ba2（Nb）Cu3O7-y cuprates doped with niobium

Polycrystalline YBa2Cu3O7-y (YBCO) and Y0.6Gd0.4Ba2-xNbxCu3O7-y (YGBNCO) compounds with 0≤x≤0.225 were synthesized using standard solid state reaction technique. The structure for all samples was characterized by X-ray difference (XRD) and scanning electron microscopy (SEM). The transport properties were measured by the (FPP) method in the temperature range from 70 to 130 K. As the Nb content in the samples increased, a diffused phase indicating a niobium perovskite phase and a small amount of unidentified phase appeared. With the increase of Nb content, the superconducting transition temperature Tconset increased slowly with x≤0.125, and then it remained unchanged or slowly decreased with 0.125≤x≤0.225. It could be found that there was a slow decrease of zero-resistance temperature, Tcoffset, with the increase of Nb content. The larger transition width might result from the YBa2NbO6 phase, impurity and unidentified phases of the sample due to the Nb doping.     

Systematic study of Ce3+ on the structural and magnetic properties of Cu nanosized ferrites for potential applications

Ce~(3+) substituted Cu-spinel nanoferrites CuCe_xFe_(2-x)O_4(x=0.00, 0.02, 0.04, 0.06, 0.08 and 0.10) were synthesized via sol-gel self-combustion hybrid route. Single phase spinel ferrite of Cu nanoferrites were examined using X-ray diffraction(XRD) analysis whereas the multiphase structure was observed as Ce contents increased from x=0.06. Field emission scanning electron microscopy(FESEM), Thermogravimetric and differential thermal analysis(TGA and DTA) and Fourier transform infrared spectroscopy(FTIR) were used to find out the morphology phase and metal stretching vibrations of Ce~(3+) substituted nanocrystalline ferrites. The crystallite size was increased and found in the range of 25-91 nm. The agglomerations in Cu ferrite samples increase as the Ce~(3+) concentration increases. The magnetic properties such as remanence, saturation magnetization, coercivity, Bohr magneton and magnetocrystalline anisotropy constant(K) were determined using M-H loops recorded from a vibrating sample magnetometer(VSM). Saturation magnetization, remanence and coercivity are increased as the Ce~(3+)contents increase in Cu nanocrystalline samples. Moreover, law of approach to saturation(LoA) was used to calculate the maximum value of saturation for Ce-doped Cu nanoferrites. The soft magnetic behaviour of the Cu nanoferrite is observed as compared to the samples substituted with the increased Ce contents in Cu nanocrystalline ferrite. Bohr magneton and magnetocrystalline anisotropy are found to increase with the substitution of rare earth Ce~(3+) contents in Cu spinel nanocrystalline ferrite. Cedoped Cu nanocrystalline ferrites with excellent properties may be suitable for potential applications in sensing, security, switching, core, multilayer chip inductor, biomedical and microwave absorption applications.     

Synthesis and Photoluminescence of BaMgAl10O17 ：Eu^2＋ Phosphor by Oxalate Co-precipitation Process

Single phase of Ba1-x MgAl10O17 ： x Eu^2＋ （0.02≤ x ≤ 0. 14） phosphors was first successfully prepared by coprecipitation in aqueous medium with a “reverse strike” method, using oxalic acid and ammonia together as precipitants. Completely crystallized phosphors were obtained at 1300 ℃, which is 300 ℃ lower than the temperature of solid-state reaction. Their photoluminescence was investigated under UV and VUV region, respectively. The emission spectra of Ba1-x MgAl10O17：xEu^2＋ samples excited by 254 or 147 nm showed a characteristic wide band with the peak centred at about 450 454 nm. Optimum emission intensity reached at x = 0.1 and then concentration quenching occurred. The synthesized phosphor shows 10% higher emission intensity than that prepared by solid-state reaction.     

Transport properties of Zintl phase Yb1-xCaxCd2Sb2 at low temperature

We investigated the transport properties of isoelectronic substitution of Yb by Ca for Zintl phase YbCd2Sb2 below 300 K.The p-type Yb1-xCaxCd2Sb2(0.2≤x≤0.8) samples were synthesized via a solid-state reaction followed by suitable cooling,annealing,grinding,and spark plasma sintering(SPS) densification processes.For samples with x=0.2,0.4,0.5,0.6,0.8,the electrical conductivity,Seebeck coefficient,thermal conductivity,heat capacity and Hall effect measurements were carried out in the temperature range from 1...     

Preparation and Ionic Conductivity of Ultrafine Li2+xRExSi1-xO3 by Sol-Gel Method

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La_(0.5)Sm_(0.2)Sr_(0.3)MnO_3/Ag_x二相复合体的结构及磁电阻

用固相反应法制备La0.5Sm0.2Sr0.3MnO3/(Ag2O)x/2(x=0.00,0.04,0.08,0.25,0.30)样品,通过X射线衍射谱线(XRD),扫描电子显微镜(SEM)照片及SEM能谱(EDS),ρ-T曲线,研究样品的输运行为及磁电阻效应。结果表明:少量掺杂时Ag全部挥发。掺杂量较多时,挥发后多余的Ag主要以金属态包覆在母体颗粒的表面,使体系形成两相复合体。掺Ag为30%摩尔比时,样品的电阻率较低掺杂样品的电阻率降低一个数量级,在300K、0.5T磁场下,磁电阻明显增强,达到9.4%,这与颗粒母体界面结构的改善有关,也与材料电阻率的降低有关。     

高频燃烧红外吸收法测定锡铅焊料中痕量硫

以硫酸钾基准试剂绘制校准曲线,将试样置于铺有0.50 g纯铁的瓷坩埚中,再覆盖3.0 g 纯钨,建立了高频燃烧红外线吸收法测定锡铅焊料中痕量硫的方法。确定最佳实验条件如下:硫质量分数不大于0.001 0%时,试样量为1.0 g; 硫质量分数为0.001 0%~0.010%时,试样量为0.50 g;硫质量分数为0.010%~0.025%时,试样量为0.20 g。结果表明,硫量在0.001 0～0.050 mg之间与其吸光度呈良好的线性关系,相关系数r=0.999 7。方法检出限为0.000 021%,测定下限为 0.000 084%。对选定的4个不同硫含量水平的锡铅焊料内控样品进行11次平行测定,测定结果与参考值基本一致,相对标准偏差(RSD)在7.3%~15.0%之间,回收率在96%~115％之间。硫质量分数在0.000 10%~0.025%之间,方法的重复性标准偏差为S_r=0.064 6 x+0.000 01、重复性限为r=0.181 2 x+0.000 03,再现性标准偏差为S_R=0.081 9 x－0.000 002、再现性限为R=0.229 7 x－0.000 006。     

Thermoelectric Properties of CexCo4Sb12 Prepared by MA-SPS

Starting with elementary powders, thermoelectric materials CexCo4Sb12 were prepared by mechanical alloying and spark plasma sintering (MA-SPS). XRD analyses reveal that the expected major phase, named skutterudite was formed in MA process and was kept after SPS. The thermoelectric properties of MA-SPS samples including resistivity, Seebeck coefficient, power factor, thermal conductivity and the dimensionless figure of merit (ZT) were studied by varying Ce content and temperature. Depending on Ce levels, both P and N types of thermoelectric semiconductors were obtained. MA-SPS sintered Ce1.0Co4Sb12 exhibits the highest ZT in the range of 100-500℃ and the maximum ZT is found at x=1.0 and 400℃.     

Effect of Ho-doping on microstructure and magnetostriction of TbDyFe alloys

Tb0.3Dy0.7HoxFe1.95 (x=0.00, 0.05, 0.10, 0.15, 0.20, 0.35, 0.50, 0.65) quaternary alloys were prepared by arc-melting and followed by annealing. The phases present and structure of the alloys were determined using a D8-Advance X-ray diffractometer. The magnetostriction of the alloys was studied by standard strain gauge technique. The dependence of Ho content on the structure, magnetostriction and density of the alloys was investigated in detail. The research results showed that Ho-doping did not change MgCu2-type cubic Laves structure in Tb0.3Dy0.7Fe1.95. When Ho content x≤0.2, rich rare earth phase presented in the alloys increased and magnetostriction of the alloys reduced evidently with increasing x, but for alloys with x>0.2, the content of rich rare earth phase started to reduce and the magnetostriction increased quickly, especially at low magnetic field in the alloy with x=0.65 due to separation of rich rare earth phases on the surface of the alloy.     

Magnetic Properties of La1-xSrxCoO3 (0≤x≤0.5)

The measurements of temperature dependence of the magnetic susceptibility of La1-xSrxCoO3 perovskite oxides at different Sr doping (0≤x≤0.5) and annealing temperature were presented. For the sample with x=0.1, a shoulder was observed around 150 K, and a peak which is one feature of spin glass appeared around 50 K in the curve of susceptibility versus temperature. The high-temperature(250～420 K)susceptibility fits well with Curie-Weiss law for all samples. Weiss constant and effective magnetic moment were determined and their variations with Sr doping and oxygen annealing condition were obtained. The Weiss constant increases monotonously with Sr content for x>0.2. The values of effective moments were interpreted with the spin state of cobalt ions. Studies on the susceptibilities of the samples with x=0.2 under different preparation temperatures and annealing temperatures show that the rising of sintering temperature and annealing temperature will increase the para-ferromagnetic transition temperature, and reduce the effective moment to normal value. Our result shows that both Co3 and Co4 ions should be in IS state after annealing and the oxygen annealing causes the transition of Co3 spin state from HS to IS.     

Effect of praseodymium substitution for lanthanum on structure and properties of La0.65-xPrxNd0.12Mg0.23Ni3.4Al0.1（X=0.00-0.20） hydrogen storage alloys

In order to investigate the effect of substituting La with Pr on structural and hydrogen storage properties of La-Mg-Ni system (AB3.5-type) hydrogen storage alloys, a series of La0.65-xPrxNd0.12Mg0.23Ni3.4Al0.1(x=0, 0.10, 0.15, 0.2) hydrogen storage alloys were prepared. X-ray diffraction (XRD), scanning electron microscopy (SEM) and energy dispersive spectrometer (EDS) analyses revealed that two alloys (x=0.0 and 0.10) were composed of (La, Mg)2(Ni,Al)7 phase, La(Ni,Al)5 phase and (La,Mg)Ni2 phase, while other alloys (x=0.15 and 0.20) consisted of (La,Mg)2(Ni,Al)7 phase, La(Ni,Al)5 phase, (La,Mg)Ni2 phase and (La, Mg)(Ni,Al)3 phase. All alloys showed, however, only one pressure plateau in P-C isotherms. The Pr/La ratio in alloy composition influenced hydrogen storage capacity and kinetics properties. Elec-trochemical studies showed that the discharge capacity decreased from 360 mAh/g (x=0.00) to 335 mAh/g (x=0.20) as x increased. But the high-rate dischargeability (HRD) of alloy electrodes increased from 26% (x=0.00) to 56% (x=0.20) at a discharge current density of Id=1800 mA/g. Anode polarization measurements were done to further understand the electrochemical kinetics properties after Pr substitution.     

RH-LF和LF-VD工艺生产管线钢洁净度的比较

比较了铁水预处理-150 t顶底复吹转炉钢水经RH-LF和LF-VD两种精炼工艺生产的管线钢(≤0.04%C-1.55%～1.78%Mn)洁净度。结果表明,RH-LF和LF-VD精炼均能使管线钢氮含量降至(30～40)×10^-6,氧含量≤10×10^-6,硫含量≤0.002 0%;LF-VD精炼渣碱度高于RH-LF精炼渣,LF-VD精炼钢平均磷含量为0.0090%,比RH-LF精炼钢低0.001 0%;两种精炼钢中主要夹杂物为钙铝酸盐和钙铝酸盐-二氧化硅复合夹杂, LF-VD精炼钢大部分夹杂物尺寸为5～10μm,RH-LF精炼钢大部分夹杂物尺寸为5～20μm。     

Magnetocaloric effect of(Tb_(1-x)Ce_x)Co_2 alloys in low magnetic field

The phases in alloys(Tb1-xCex)Co2 with x=0,0.1,0.2,0.3,0.4 and 0.5 were investigated by X-ray diffraction analysis,and the magnetocaloric effect for x=0-0.4 was studied by magnetization measurement.The samples were almost single phase with MgCu2-type cubic structure.The magnetization decreased with the increase of Ce.The Curie temperatures(Tc) of Tb1-xCexCo2 alloys with x from 0.1 to 0.4 were 180,165,160 and 152 K,respectively.For x=0.5 in the range from 100 K to 230 K,the point of magnetic transition was n...     

钛含量对Nb-Ti微合金化Q345A钢热轧板力学性能的影响

试验研究了钛含量对Q345A钢(%:0.08～0.10C、1.19～1.46Mn、0.017～0.029Nb、0.02～0.08Ti) 14～20mm热轧板力学性能的影响。结果表明,Ti=0.02%时,钢板的强度无显著变化,Ti为0.02%～0.04%时,钢板强度随Ti含量增加而增加;Ti≥0.04%时,钢板强度随Ti含量增加而下降。控制Nb-Ti微合金化重型汽车板用钢Q345A的Ti含量为0.02%～0.04%,可获得最佳强塑性配合。     

The role of the neurotransmitters acetylcholine and noradrenaline in the pathogenesis of stress ulcers

Molecular self-diffusion coefficients of water (0.75 +/- 0.05), N-acetylaspartate (0.27 +/- 0.04), creatines (0.27 +/- 0.04), and cholines (0.28 +/- 0.08) x 10(-5) cm2 s-1 were obtained from localized proton NMR spectra of rat brain in vivo using diffusion-weighted stimulated-echo (STEAM) sequences with a diffusion time of (delta--delta/3) = 17 ms.     

BOF-LF-RH-CC流程高压锅炉管用钢12Cr1MoVG的生产实践

φ110 ～ φ280 mm锅炉管用热轧圆钢12Cr1MoVG(/％:0.08 ～0.15C、0.17 ～0.35Si、0.40 ～0.70Mn、≤0.015P、≤0.010S、0.90 ～ 1.20Cr、0.25 ～0.35Mo、0.15 ～0.30V、≤0.015[Alt])的生产工艺流程为120 t顶底复吹转炉-LF-RH-CC-轧制.通过控制铁水[As]、[Sn]、[Sb]、[Pb]、[Bi],控制转炉终点[C]0.04％ ～0.08％、[P]≤0.010％、[S]≤0.010％,出钢过程铝铁脱氧,钢包喂铝线控制[Alt]≤0.015％并用复合精炼渣和少量铝丸终脱氧,控制中间包钢水过热度20 ～35℃,全程保护浇注等工艺措施,使试验钢的[As]+[Sn]+[Sb]+[Pb]+[Bi]≤0.029％、[P]≤0.011％、[S]≤0.008％、[Alt]≤0.011％,各类夹杂物级别均≤1.0,满足用户的技术要求.     

Synthesis and characterization of Gd-doped PbMoO_4 nanoparticles used for UV-light-driven photocatalysis

Gd-doped PbMoO_4 nanoparticles were prepared by a refluxing method at 80℃ for 2 h.Effect of molar content of Gd dopant on phase,morphology and optical properties was studied.The as-prepared Gddoped PbMoO_4 samples can be indexed to pure tetragonal PbMoO_4 phase.The particles size of PbMoO_4 is decreased with increasing in the molar content of Gd dopant from 15.20±3.04 nm for pure PbMoO_4 to 8.72±1.53 nm for 5 mol% Gd-doped PbMoO_4.The absorption of 5 mol% Gd-doped PbMoO_4 nanoparticles shows red-shift caused by lattice distortion of PbMoO_4.The photocatalytic performance of 5 mol% Gddoped PbMoO_4 nanoparticles shows the highest degradation of rhodamine B(RhB) of 97.92% under UV radiation and 67.65% under visible radiation because Gd~(3+) dopant as an electron acceptor plays the role in enhancing the separation of electron-hole pair.     

Optimal control of intermittent normal conduction in a tachycardia-dependent right bundle branch block

Tachycardia-dependent right bundle branch block (RBBB) with atrial fibrillation in a patient under digitalis therapy is presented, in which supernormal phase of intraventricular conduction was well-documented. The development of long intervals terminated by a normally conducted beat was attributed to the occurrence of concealed atrio-ventricular (A-V) conduction of the atrial fibrillation impulse during the supernormal phase. The ventricular interval caused by a normally conducted beat (xs) in the interval of 1.01-1.63 s was transformable into a vector differential equation dy/dx = In (x + a) + 1, where parameter a = 0, 0.04, 0.08, 0.16, and 0.24. This is piecewise continuous and integrable. The function in (x + 0.04) + 1 was considered to give the solution of the problem of optimal control, which is equivalent to the problem of finding Green's function of the region, i.e. to solving the Dirichlet problem. The solution curves, given by y = (x + a) in (x + a) + 1, can be interpreted as distributions. There were structurally stable vector field points on a differentiable manifold, i.e, attractors. In general, the modelling may be applicable to tachycardia-dependent RBBB.     

Catalytic Activity of Ceria-Zirconia Nanostructured Materials Prepared via Reversed Microemulsion Method

CeO2-ZrO2mixed oxides have a number of i mpor-tant catalytic applications[1].They are extensively em-ployed in current automotive three-way catalysts(TWCs)as the oxygen storage promoters,i.e.materi-als that regulate the oxygen partial pressure throughtheC…     

Phase Structure and Electrochemical Properties of Rare Earth Based Hydrogen Storage Alloys

The rare earth based hydrogen storage alloys MmxM1 1 - x ( Ni3.55 Co0.75 Mn0.4 A10.3 ) ( x = 0 ～ 0.5 ) were investigated in this work.Adjusted Ml: Mm ratio to change the content of La,Ce,Pr and Nd in the alloys and then to change the phase structure, the influences of phase structure on the electrochemical properties were analyzed.The results indicate that the main phase of all alloys is LaNi5 with CaCu5 type structure and the crystal lattices constants of LaNi5 are changed with increasing x value, i.e, decreased a-axis, increased c-axis and axis ratio and nonlinear decreased crystal volume.The crystal volume of the alloy with x = 0.3 is larger than others.There is second phase A1LaNi4 in alloys when x≥0.3, which decrease the discharge capacity, but increase the cycling stability and high rate discharge ability.Compared comprehensively, the alloy with x = 0.3 shows the higher discharge capacity and the better cycling stability.