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1.
利用MgF_2作为扩散源进行镁离子内扩散LiNO_3单晶基片的研究.经电子探针显微镜分析表明,镁的扩散层镁离子浓度分布具有近似半抛物形和阶跃形分布,并得到镁的激活能为104KJ/.X射线衍射分析发现,当镁离子内扩散超过一定程度时,在镁的扩散层出现具有LiNb_3O_8的物相结构,并发现该物相结构的出现与LiNO_3体内锂离子的外扩散和扩散表面氟离子的存在有关.由扫描电子显微镜观察到氟离子以LiF的形式出现,并随着扩散程度的增大,挥发和脱离开扩散层表面.  相似文献   

2.
陈昂  智宇  戴希  鲍亚华  杨敬思 《物理学报》1994,43(12):2038-2044
报道了超导陶瓷YBa2Cu36+δ与铁电陶瓷BaTiO3进行复合的结果。研究了该复合功能陶瓷的物相、(超)导电性和低温电阻温度特性。结果表明,采用合理的合成工艺,可得到呈现混和分布的两相复合功能陶瓷材料;该复合材料的电导特征符合三维渗流导电行为,发现在较高YBa2Cu36+δ含量时,样品呈超导电性,并对此作了初步讨论。 关键词:  相似文献   

3.
陈志雄  黄卓和  何爱琴  石滨 《物理学报》1994,43(6):1035-1040
在通常的ZnO-Bi23-Sb23系电压敏陶瓷中,加入能构成压敏特性的钡添加剂,发现除已知的Bi23和Zn2.33Sb0.674晶界相以外,还出现新的晶界相,分析表明是固溶有微量其它成分的偏锑酸钡(BaSb26)晶相。同时还发现,BaSb2关键词:  相似文献   

4.
用内转换电子穆斯堡尔谱(CEMS)和慢正电子束研究了含3%Y23的ZrO257Fe离子(100keV,3×1016at./cm2)注入态及其在氢气氛中退火的热力学行为.注入态以Fe3+,Fe2+和Fe0存在,它们分别是Fe3+-V(空位)复合体、二聚体和超顺磁颗粒.经400,500℃退火后,Fe3+-V分解,分别出现了α-Fe的前期相和α-Fe纳米颗粒.含Fe的ZrO2(Y)混合导电的出现可能是和Fe的不同价态及其相对含量有关 关键词:  相似文献   

5.
崔彩娥  王森  黄平 《物理学报》2009,58(5):3565-3571
采用溶胶凝胶法制备了Sr3Al26:Eu2+,Dy3+红色长余辉发光材料,利用X射线衍射仪对材料的物相进行了分析,结果表明,1200℃下制备的样品的物相为Sr3Al26,少量的Eu和Dy掺杂没有影响样品的相组成.采用荧光分光光度计、照度计测定了样品的发光特性.结果表明Sr3Al2关键词: 红色长余辉 3Al26')" href="#">Sr3Al26 溶胶凝胶法  相似文献   

6.
曹效文  唐元冀  何健民 《物理学报》1994,43(11):1854-1859
系统地研究了R1-xPrxBa2Cu37-δ的超导Tc与Pr替代浓度x的关系。发现在离子半径ri≤ri(Dy)时,在低Pr浓度范围内存在一个超导Tc平台,并且平台宽度表明一个R3+离子尺寸效应。我们认为,Tc平台宽度的离子尺寸效应可能起源于Pr4f电子局域态的改变。提出一个临界R3+离子半径ric,ri>ric时RBa2Cu37-δ的超导电性消失 关键词:  相似文献   

7.
杨春  冯玉芳  余毅 《物理学报》2009,58(5):3553-3559
采用基于第一性原理的从头计算分子动力学方法,计算了300—800℃下AlN吸附过程与系统能量、动力学轨迹以及扩散系数.研究表明,吸附过程由物理吸附、化学吸附和表面稳定态三个阶段组成,在吸附成键过程中,温度越高,粒子平均表面扩散能力增强.N原子的扩散系数大于Al原子的扩散系数,尤其是在物理吸附阶段.在较高温度条件下(大于700℃),N的解吸附作用明显增强,不利于AlN的稳定吸附生长,500—700℃之间的温度有利于AlN在α-Al23(0001)表面的稳定吸附生 关键词: 2O3(0001)表面')" href="#">α-Al23(0001)表面 扩散 吸附生长 从头计算分子动力学  相似文献   

8.
秦毅  张辉  谈松林  刘婷  张鹏翔 《物理学报》2009,58(5):3497-3502
采用脉冲激光沉积(PLD)镀膜技术在倾斜10°的LaAlO3(100)单晶衬底上制备了(SrTiO3n/(SrTi0.8Nb0.23m系列超晶格.在超晶格薄膜的XRD图谱中清楚地观察到周期调制的卫星峰结构.从卫星峰的分布计算了超周期,进而得到了在生长SrTiO3和SrTi0.8Nb0.2< 关键词: 3n/(SrTi0.8Nb0.23m]20/LAO(100)超晶格')" href="#">[(SrTiO3n/(SrTi0.8Nb0.23m]20/LAO(100)超晶格 激光感生热电电压 各项异性Seebeck系数 原子层热电堆  相似文献   

9.
苏昉  王文楼  谢斌  蒋宗驷  林枫凉 《物理学报》1994,43(10):1648-1657
用混溶蒸发法制备出高聚物(PEO)n-CuBr2(n=4,8,12,16,24)薄膜。并详细测量它们在0.1-350MPa静水压范围的复阻抗谱,以及在0.1-2400MPa静水压范围的交流电导率。结果表明:离子电导率与压力的依赖关系可分解为四段相迭加的线性关系。根据X射线衍射物相分析,它们分别归于PEO非晶相的压力效应,PEO结晶相的压力效应和析出新相CuBr2的压力效应。最后给出克服办法——添加少量增塑剂碳酸乙烯酯可增加(PEO)n-CuBr2薄膜的弹性,使压力下的离子电导率提高一至两个数量级。 关键词:  相似文献   

10.
Gd1-xCaxBa2Cu3O7-y高温超导体压力效应的研究   总被引:1,自引:0,他引:1       下载免费PDF全文
韩翠英  方芳  解思深 《物理学报》1994,43(10):1704-1711
研究了Gd1-xCaxBa2Cu37-y(0.0≤X≤0.20)高温超导体在常压和高压下的超导电性在1-300K温度范围内,利用Bridgman对顶砧获得压力达9.0GPa,测量了(X=0.10,0.15,0.20)样品的dTc/dp分别为7.68,7.8和4.46K/GPa。发现Tc的压力导数随着ca2+含量的增加而下降,分析了氧含量对Tc和dTc/dP的影响.利用常压下晶格参数精修值和阳离子与氧离子间距随压力的改变,说明CuO2面在超导电性上的作用,用CuO2面之间耦合解释Tc(P)曲线的非线性关系。 关键词:  相似文献   

11.
阙文修  姚熹 《物理学报》1996,45(5):811-816
利用常规X射线衍射和掠入射X射线衍射对在空气中进行镁离子内扩散的扩镁铌酸锂单晶表层的富氧化镁层特性进行了研究,揭示出镁离子内扩散初期随着体内锂离子的外扩散,首先在富氧化镁层形成Li3Mg2NbO6和Mg4Nb2O9的化合物结构,Li3Mg2NbO6出现在富氧化镁的内表层,而Mg4Nb关键词:  相似文献   

12.
阙文修  霍玉晶 《光学学报》1995,15(7):44-947
利用镁离子内扩散的方法,实现了铌酸锂单晶光纤具有抛物型折射率包层的波导结构。对扩散层中的镁离子浓度分布进行了理论模拟,理论和实验结果相符合。  相似文献   

13.
Several chemical compounds based lithium niobate have been tested in the reaction for the photocatalytic hydrogen generation. The photocatalysts have been prepared by impregnation of Nb2O5 in the aqueous solution of lithium hydroxide and then the calcination at the temperature range of 400-650 °C. In this report, we present the interesting study showing that the most active catalyst for the photocatalytic generation of hydrogen is the one containing two lithium niobate phases such as LiNbO3 and LiNb3O8. It means that the lithium niobates based catalyst without any further modification or doping can be applied as a novel material for this process.  相似文献   

14.
The electrochemical performances of LiNi0.5Co0.2Mn0.3O2 (NCM523) layered cathode material, such as poor rate capacity and cycling stability caused by undesirable intrinsic conductivity and low rate of lithium ion transportation, are not fairly good especially at elevated rate and cut-off voltage. To improve these properties, in this study, the co-coating layer of graphene and TiO2 was constructed on NCM523 surface. The graphene/TiO2 coating layer could effectively prevent hydrofluoric acid (HF) attacks, suppress the side reaction, accelerate the lithium ion diffusion and facilitate the electron migration. The enhancement of cycle performance and rate capacity was contributed to the uniform co-modified surface, interacting each other and thus exhibiting synergistic effects.  相似文献   

15.
Epitaxial Fe3O4(0 0 1) thin films (with a thickness in the range of 10-20 nm) grown on MgO substrates were characterized using low-energy electron diffraction (LEED), conversion electron Mössbauer spectroscopy (CEMS) and investigated using Rutherford backscattering spectrometry (RBS), channeling (RBS-C) experiments and X-ray reflectometry (XRR). The Mg out-diffusion from the MgO substrate into the film was observed for the directly-deposited Fe3O4/MgO(0 0 1) films. For the Fe3O4/Fe/MgO(0 0 1) films, the Mg diffusion was prevented by the Fe layer and the surface layer is always a pure Fe3O4 layer. Annealing and ion beam mixing induced a very large interface zone having a spinel and/or wustite formula in the Fe3O4-on-Fe film system.  相似文献   

16.
A novel Y-branch waveguide for power dividing and mode splitting   总被引:1,自引:0,他引:1  
A novel Y-branch waveguide for variable-ratio power dividing and transverse electrical-transverse magnetic (TE-TM) mode splitting depending on the applied voltage is presented. The Y-branch waveguide is formed by two closely coupled waveguides tabricated by nickel indiffusion (NI) and by magnesium-oxide induced lithium outdiffusion (MILO) in a y-cut lithium niobate (LiNbO3) substrate. The TE component of the randomly polarized light is tuned between these two waveguides, such that the device can be either a power divider or a mode splitter depending on the applied voltage. The measured TE mode extinction ratio is about 20 dB.  相似文献   

17.
We report experimental observation of ultra-long lifetime UV-induced absorption in undoped and 5 mol.% Mg-doped congruent lithium niobate crystals between 400 nm and 2500 nm wavelength range. The saturated absorption coefficient change in undoped congruent lithium niobate was about 3 to 7 times that in Mg-doped congruent lithium niobate in the mid-infrared spectrum. The UV-illuminated LiNbO3:Mg was fully recovered in the dark after 2 days, whereas the undoped congruent LiNbO3 still exhibited nontrivial infrared absorption. We attribute the cause of the UV-induced absorption to the creation of hole-trapped intermediate states O near lithium vacancies.  相似文献   

18.
The glass composition (90?mol% Li2B4O7–10?mol% Nb2O5) was prepared by the melt quenching technique. The quenched sample was heat treated at 480°C, 545°C and 630°C for 5?h and heat treated at 780°C with different time. The times were 5, 10, 15, 20, 28, and 36?h. The glass and glass ceramics were studied by differential thermal analysis (DTA), X-ray diffraction (XRD), and dc conductivity as a function of temperature. Lithium niobate (LiNbO3) and lithium diborate (Li2B4O7) were the main phases in glass ceramic addition to traces from LiNb3O8. Crystallite size of the main phases determined from the X-ray diffraction peaks are in the range <100?nm. The fraction of crystalline (LiNbO3) phase increases with increase the heat treatment temperature and time. The relation between physical properties and structure were studied.  相似文献   

19.
胡伯清  周棠  田万春 《物理学报》1983,32(8):1098-1103
本文测定了LiNb3O8晶体的透光曲线,肯定了晶体发黑的主要原因是氧空位,以及通过退火消除的方法;确定了晶体中氢键形成的原因是大气中水蒸汽和熔体起反应的结果,真空退火是消除氢键的方法;提出了在纯氧气氛下生长LiNb3O8晶体的建议;测定了LiNb3O8晶体的光性方位和主折射率,并和LiNbO3晶体作了比较;讨论了LiNb3O8晶体的光性方位和它的结构关系。 关键词:  相似文献   

20.
X-ray photoelectron spectroscopy has been applied to interface studies of Ag/tris-(8-hydroxyquinoline) aluminum (Alq3) and Ag/LiF/Alq3. For Ag/Alq3, diffusion of Ag atoms into the Alq3 layer occurs immediately after the adhesion of the metal onto the organic layer and the process lasts several hours. Insertion of a monolayer-thick LiF buffer at the interface can effectively block the diffusion process. This is quite different from what is observed from Al/LiF/Alq3, where Al penetrates into the LiF layer as deep as several nanometers. It is thus concluded that the LiF buffer may play different roles in Ag/LiF/Alq3 and Al/LiF/Alq3 and hence different mechanisms may dominate in the two cases for the enhanced carrier injection observed.  相似文献   

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