Tm3+掺杂锗铌酸盐玻璃及其红外光谱特性

用高温熔融法制备了相同质量百分比浓度4%Tm₂O₃掺杂浓度下(90-x)GeO₂-xNb₂O₅-10Na₂O(其中数字为摩尔百分比x=1,2,4,6,8)以及Tm₂O₃掺杂浓度分别为质量百分比1%,2%,3%,4%下86GeO₂-4Nb₂O₅-10Na₂O(其中数字为摩尔分数)系列玻璃.研究了Nb₂O₅组分对玻璃热稳定性,荧光强度和J-O参数的影响.应用Judd-Ofelt理论,计算了Tm³⁺离子在Nb₂O₅浓度不同时的J-O强度参数(Ω₂,Ω₄,Ω₆)及Tm³⁺离子各激发态能级的自发跃迁概率、荧光分支比以及辐射寿命等光谱参量.根据McCumber理论,计算了Tm³⁺离子能级³F₄→³H₆(1.8 μm)跃迁的吸收截面和受激发射截面.从获得的吸收截面、发射截面与离子掺杂浓度计算了1.8 μm荧光波段的增益截面曲线.在808 nm波长光的激发下,研究了Tm³⁺掺杂玻璃在1.47与1.8 μm附近的荧光特性.发现当Tm₂O₃掺杂浓度为质量百分比3%时,在1.8 μm处的荧光强度达最大,然后随着掺杂浓度的增大,其荧光强度反而降低;当Nb₂O₅摩尔分数含量大约在2%时,Tm³⁺在1.8 μm处的荧光强度最强.并讨论了Nb₂O₅组分变化对玻璃结构与光谱特性的影响情况. 关键词： 3+掺杂锗铌酸盐玻璃')" href="#">Tm³⁺掺杂锗铌酸盐玻璃 红外光谱性质 交叉弛豫 2O₅')" href="#">Nb₂O₅     

B2O3含量对掺铒碲铌酸盐玻璃光谱性质及热稳定性影响

制备了一系列碲铌酸盐玻璃85TeO₂-(15-x)Nb₂O₅-xB₂O₃-1%Er₂O₃(TNBx=0, 3, 6, 9, 12, 15).根据Judd-Ofelt(J-O)和McCumber理论,讨论和分析了B₂O₃含量对掺铒碲铌酸盐玻璃热稳定性及光谱性质影响.研究发现,玻璃开始析晶温度和玻璃转变温度差值ΔT(T_x-T_g),J-O强度参数,FWHM和峰值受激发射截面的乘积在B₂O₃引入摩尔分数为9%时达到最大值.同时,Er³⁺:⁴I_13/2能级寿命也随着B₂O₃含量的增加而单调增加.结果表明,在掺铒碲铌玻璃中,适量的B₂O₃能较好地提高玻璃的热稳定性能和Er³⁺离子的光谱性质.     

Li2O-Nb2O-SiO2系统非晶态离子导体的结构与电学性能

本文采用红外吸收光谱法、X射线散射法和EXAFS方法研究了LiO-Nb₂O-SiO₂系统非晶态离子导体的结构,认为Nb⁵⁺在非晶结构网络中主要是以[NbO₆]形式存在。非晶结构随Nb₂O₅含量的多少而变化。低Nb₂O₅含量时,[NbO₆]相互间以边相连,并与[SiO₄]组成多元环后,形成非晶网络结构。高Nb₂O₅含量时,非晶网络结构主要是以角顶相连的[NbO₆]所组成。根据电导测试结果,讨论了结构与电学性能的关系,认为Li₂O含量在0.45左右,Nb₂O₅,含量在0.3左右组成的非晶材料有最高的电导率。 关键词：     

CeO2/Nb2O5界面效应对提高CeO2氧敏特性的XPS研究

用射频/直流磁控溅射法制备了CeO₂/Nb₂O₅双层氧敏薄膜，利用X射线光电子能谱(XPS)，描述并解释了单层CeO₂薄膜中氧随温度变化的动力学行为，以及CeO₂/Nb₂O₅薄膜界面对氧敏特性的影响.通过对Ce3d XPS谱的高斯拟合，计算了Ce³⁺浓度并给出了判定Ce⁴⁺还原的标志.结果表明，界面效应可以提高CeO₂/Nb₂O₅薄膜中Ce⁴⁺的还原能力，使之远远高于单层CeO₂薄膜，这对薄膜的氧敏特性是极为有利的. 关键词：     

氧化铝与Al(100)基体间界面原子结构研究

本文介绍了用MeV离子散射和沟道效应研究单晶铝表面无定型氧化层与基体之间界面原子结构的方法。报道了Al₂O₃/Al(100)界面原子结构的实验结果。实验表明,在纯氧气氛围中400℃下生成的氧化铝膜,铝和氧原子浓度比例严格为2与3之比;Al₂O₃膜和Al(100)基体之间的界面极其陡峭,氧化铝膜下Al(100)基体表面的再构层不大于一个原子层。由实验测量与用Monte Carlo方法计算结果比较,得到再构层原子离开原来晶 关键词：     

改进铜铌溅射型QWR超导腔性能的探讨

通过直流偏压二级溅射方法，在无氧铜腔体表面溅射一层铌膜，研制了铜铌溅射型射频超导1/4波长谐振腔(quarter wave resonator,QWR)，该腔主要用于重离子的加速，是北京放射性核束装置中后加速部分的预研项目.目前国际上很多实验室都在研究进一步提高铜铌溅射型QWR超导腔的性能，通过多种方法的实验研究，发现在无氧铜衬底与铌膜之间加入一层氮 化铌（NbN）薄膜，可以使得表面铌膜的超导温度转变点由原来的8.8K提高到了接近9.6K ，该方法有可能成为提高QWR腔加速性能的重要途径，目前进一步研究正 关键词： 溅射 QWR超导腔 氮化铌NbN 超导温度     

多孔CeO2膜的制备及其光谱性能

以铈箔为原料,采用阳极氧化法和热处理法制备多孔的CeO₂膜。将阳极氧化铈膜分别在400,500和800 ℃下进行热处理,分别研究阳极氧化铈膜的晶体结构、组成和表面形貌,分别研究多孔的CeO₂膜红外光谱特征吸收和热膨胀性能。阳极氧化铈膜是Ce(OH)₃,CeF₃,Ce₂O₃,CeO₂和Ce的混合膜,并吸附水和乙二醇,其中Ce(OH)₃,CeF₃,Ce₂O₃分别为六方晶型结构,CeO₂和Ce分别为立方晶型结构。阳极氧化铈膜中的Ce(OH)₃,Ce₂O₃和Ce分别在400和500 ℃进行热处理时可能分别转变为CeO₂,分别在400和500 ℃热处理后的膜为CeF₃和CeO₂的混合膜。阳极氧化铈膜中的Ce(OH)₃,CeF₃,Ce₂O₃和Ce在800 ℃进行热处理时可能分别转变为CeO₂,在800 ℃热处理后的膜为CeO₂膜。该CeO₂膜是多孔的膜,且孔为直孔,在1 600～4 000 cm-1范围内具有强吸收。该CeO₂膜在170～900 ℃范围内热膨胀系数变化不大,该膜的热稳定性较好。     

铁氧化物中电子隧道现象的扫描隧道显微术研究

报道了利用扫描隧道显微术(STM)对金属表面氧化物层进行电子隧道谱研究的结果。在对两类铁晶体表面氧化层进行的隧道谱和势垒高度测量结果进行分析后表明,常温条件下形成的氧化层(Ⅰ类)应主要是Fe₃O₄;而在高温氧化条件下形成的表面层(Ⅱ类)的主要成分则应是Fe₂O₃。从而表明(STM)可用于研究铁表面氧化过程的不同阶段,并且由Ⅰ类氧化层的低势垒特性说明STM还可以用于观测此类氧化层的内部结构。类似研究方法还可应用到对一系列 关键词：     

离子束溅射制备Nb2O5光学薄膜的特性研究

研究了离子束溅射(IBS)制备的Nb₂O₅薄膜的光学特性、应力、薄膜微结构等特性,系统地分析了辅助离子源的离子束能量和离子束流对薄膜特性的影响.结果显示,在辅助离子源不同参数情况下,折射率在波长550 nm处为2.310—2.276,应力值为-281—-152 MPa.在合适的工艺参数下,消光系数可小于10^-4,薄膜具有很好的表面平整度.与用离子辅助沉积(IAD)制备的薄膜相比,IBS制备的薄膜具有更好的光学特性和薄膜微结构. 关键词： 2O₅薄膜')" href="#">Nb₂O₅薄膜 离子束溅射 光学特性 应力     

用于α-Al2O3分子动力学模拟的长程Finnis-Sinclair势函数

用金属势函数描述氧化物是实现金属-氧化物界面分子动力学模拟的关键.基于此,通过拟合α-Al₂O₃的晶格能、晶格常数、弹性常数,获得了一套用于描述α-Al₂O₃的长程Finnis-Sinclair（F-S）势.通过与已报道的描述α-Al₂O₃的EAM势、Glue势和modified Matsui（m-Matsui）势的比较,结果达到或优于前人的结果.进而,在300 K的温度下对 关键词： 长程F-S势 2O₃')" href="#">α-Al₂O₃ 2O₃界面')" href="#">Fe-Al₂O₃界面 2O₃界面')" href="#">Al-Al₂O₃界面     

Nb3Sn复合超导体晶粒生长机制

本文研究了Nb/固态Cu-Sn和Nb/液态Cu-Sn界面上Nb₃Sn晶粒的生长。实验表明:固态-固态界面上生长的晶粒尺寸虽小(约0.1μm),但Nb₃Sn晶粒的长大仍符合通常的固态晶粒长大规律;固态-液态界面上生长的Nb₃Sn分成两层,靠近Nb的内层晶粒细小,排列致密,外层晶粒粗大,分布零散,后者是前者经过溶解/沉积过程引起的,晶体形貌大多数呈菱形十二面体,部分呈正交平行六面体,说明Nb₃Sn的{110},{100}面     

Die Übergangstemperatur verschiedener Supraleiter zweiter Art unter hydrostatischem Druck

An apparatus for production of hydrostatic pressure is described using a mixture of n-pentane and iso-pentane, which transmits pressure uniformly still at low temperatures. The superconductive transitions of the A 15(β- W type)-compounds Nb₃Sn, Nb₃Al, V₃Si and the B 1(NaCl type)-compound NbN have been measured under pressure up to 18 · 10³ kp/cm². The transition temperatures of the compounds V₃Si and NbN are increasing with pressure. Further measurements have been done on some selected ternary compounds, e.g. Nb₃(Al_1?x Ge _x ), to prove some predictions for the effect of pressure on superconductive transition.     

Auger electron spectroscopic study of the surface oxidation of uranium-niobium alloy {U-6 wt.% Nb} in a UHV environment containing primarily H2, H2O and CO

Auger electron spectroscopy has been used to study the surface oxidation of a uranium-niobium alloy, U-6 wt.% Nb, in a UHV environment containing primarily H₂, H₂O and CO. For comparison, the reaction of the oxidative species with pure uranium and niobium metals has also been investigated. The observed changes of the shape and position of the Auger transition peaks for U, Nb and O following exposures this UHV environment up to 200 L, and under a continuous electron bombardment indicated that oxidation of the alloy leads, first, to the formation of a surface oxide consisting of UO_2.0. The formation of this oxide was followed by the development of Nb-oxides (NbO, NbO₂ and Nb₂O₅) at the metal-oxide interface. Pure uranium was found to exhibit faster oxidation kinetics than the alloy, while pure niobium oxidised at a much lower rate than the uranium based materials.     

合金元素对Nb3Sn生长动力学的影响

研究了合金元素Zr对Cu-Sn/Nb界面上Nb₃Sn生长动力学的影响。实验表明:在单芯复合材料中加入Zr显著提高了Nb₃Sn层的生长速率,层厚与时间的关系显著超过抛物线规律。这些结果不能仅用内氧化生成的ZrO₂颗粒使晶粒细化来解释,还必须考虑ZrO₂颗粒周围过饱和空位使扩散系数增大等因素。在多芯复合材料中热处理时Cu-Sn基体中Sn量的消耗,显著影响Nb₃Sn的生长。考虑了这一因素的Nb₃Sn生长动力学修正公式能对实验结果进行解释。 关键词：     

Nb/Nb3Sn复合超导材料的高压电子显微镜观察

用1000kV高压电子显微镜观察了单芯和多芯Nb/Nb₃Sn复合材料的显微组织,看到了由Nb₃Sn/Nb₃Sn晶粒重叠而成的叠栅图和Nb基体/Nb₃Sn晶粒重叠而成的叠栅图。 关键词：     

Surface sprouting growth of Na2Nb2O6·H2O nanowires and fabrication of NaNbO3 nanostructures with controlled morphologies

The one-dimensional (1D) Sandia octahedral molecular sieves (SOMS) Na₂Nb₂O₆·H₂O nanowires were prepared by the reaction of Nb powder with NaOH via a one-step hydrothermal methods. The products were characterized by SEM, TEM, XRD, IR and EDX. A plausible sprouting growth mechanism is proposed for the formation of Na₂Nb₂O₆·H₂O nanowires based on the systematic investigation. Na₂Nb₂O₆·H₂O nanoribbons-based complex flowerlike structure were first grew on the metallic niobium surface, the growth process of SOMS nanowire is similar to the plant seed sprouting and growing, Na₂Nb₂O₆·H₂O nanowires were finally formed at the depletion of metallic niobium powder. In the end, we showed that Na₂Nb₂O₆·H₂O nanowires is hydrothermally synthesized in the 15 M NaOH solution at 423 K, which can be easily converted into NaNbO₃ nanowires by calcination, while the NaNbO₃ cubes were obtained through the same hydrothermal process at a higher temperature of 453 K.     

Ion-beam reduction of the surface of higher niobium oxide

X-ray photoelectron spectroscopy is used to study the process of reduction of the surface of the higher oxide Nb₂O₅ upon bombardment with inert gas ions (Ar⁺) and reactive gas ions (O₂⁺) with an energy of 1 and 3 keV in high vacuum at room temperature. It is found that, upon bombardment with Ar⁺ ions, the lower oxide NbO and the intermediate oxide NbO₂ are formed in the surface layers of the oxide Nb₂O₅. Bombardment with O₂⁺ ions leads to the formation of an extremely insignificant amount of the intermediate oxide NbO₂ in the surface layers of the oxide Nb₂O₅. It is revealed that the process of ion-beam reduction of the surface of the oxide Nb₂O₅ depends on the ion type, dose, and energy of exposure.     

Synthesis and Characteristics of Ultra-Fine Superconducting Powders in the Nb–N,Nb–N–C,Nb–Ti–N–C systems

The single phase powders of NbN, NbN_1-yC_y, Nb_1-xTi_xN_1-yC_y with a mean particle size of 10–70nm were prepared in the nitrogen plasma flow of a microwave discharge at a hydrogen reduction of NbF₅ only, or in a mixture with C₅H₁₂, or with the addition of TiCl₄. It was established that the critical magnetic field of ultra-fine niobium–titanium carbonitride powders is about three times higher as compared with bulk samples of the same composition. The critical magnetic field ran up to 55T for ultra-fine powders with the optimal composition Nb_0.8Ti_0.2N_0.8C_0.2. This material may be interesting for the technical superconductivity in the helium temperature range.     

An ab initio study of niobium (n = 2--11) clusters: structure, stability and magnetism

The ground-state configurations of the Nbn (n = 2-11) clusters are studied through the first-principles calculations. It is found that niobium clusters (n = 2-11) tend to form compact structures with low symmetry. The clusters with 4, 8 and 10 atoms are found to be magic and have relatively large highest occupied-lowest unoccupied molecular orbital (HOMO-LUMO) gaps. The Nbn clusters possess low magnetic moments, which exhibit an odd-even oscillational character. The analyses of calculated electronic density and population of the lowest-energy niobium clusters for n = 2, 3, 5, 7, 9, 11 show that the total magnetic moments of Nbn originate mainly from a few Nb atoms with longer spacings between them in most cases, while they are located on two Nb atoms for n = 2, 3, 5. The total magnetic moments come mainly from the 4d local moments but with the exception of the Nb5 cluster.     

X-ray spectra and electronic structure of Li x NbO2 superconductor and other niobium oxide compounds

X-ray emission Nb and OK spectra and O1s total photoelectron yield spectra for superconductor Li_0.71NbO₂ and other niobium oxide compounds NbO, BaNb₄O₆, Ba₂Nb₅O₉, BaNb₅O₈. LiNbO₂, NbO₂, LiNbO₃ were investigated. It was found that in stoichiometric LiNbO₂, niobium oxidation degree is 3+. Under the lithium deintercalation down to Li_0.71NbO₂ composition, the niobium ions oxidation degree increases up to 3.3+. As more electrons are supplied by Nb to fill the O2p band, the degree of O2p-Nb4d hybridization is increased. Using the full-potential linear muffin-tin orbital method, the self-consistent band structure calculations of Li _x NbO₂ (x=1.0; 0.7; 0.5) compounds were carried out. Agreement between partial Nb4d and O2p densities of states and corresponding X-ray spectra was observed. For thex=0.7; 0.5 the Fermi level is placed on the slope of sharp density of states peak formed mostly by the Nb4d states. With the decrease ofx thep-d hybridization becomes stronger, although remains well below the values typical for the high-temperature superconductors.