Bi-1212相和Bi-1222相铜氧化合物的合成和超导电性

对名义组份为(Bi_(1-x),M_x)Sr_2YCu_2O_y(x=0.6—0.7)的样品,当M=Cd,Ni和Zn时合成了Bi-1212相材料,实验发现Cd占据Bi位,可以稳定单BiO层,高压氧下退火,在32K出现超导转变,而Zn和Ni进入CuO平面,占据Cu位,破坏了材料的超导电性。用Cd稳定单BiO层还能够合成Bi-1222相化合物,它的固溶范围比Bi-1212大,对这一现像进行了结构上的分析。在不同氧压退火处理下的Bi-1222相样品,电阻随氧压增大而变小,但在4.2K以上未观察到超导转变。 关键词：     

CRYSTAL STRUCTURE INVESTIGATION OF VANADYL COMPLEXES OF TRIDENTATE LIGAND (Ⅰ)——THE CRYSTAL STRUCTURES OF BIS[(1-(2,4-PENTANE- DIONATO(NITROBENZOYL) HYDRAZONE)-2- ETHOXY)OXOVANADIUM] AND BIS-[(1-(2, 4-PENTANEDIONATO-(3-NITROBENZOYL) HYDRAZONE)-2- METHO

The title complexes were obtained by the reactions of bis(2,4-pentanedionato)oxovanadium VO(Acac)_2 and m-nitrophenylhydrazide m-NO_2PhCONHNH_2 in the media EtOH and MeOH respectively. The compound (Ⅰ) crystallizes in the space group PT with unit cell dimensions a=8.123(2), b=10.409(5), c=10.822(4), α=65.78(3)°, β=85.50(3)°,γ=89.04(3)°. The compound (Ⅱ) crystallizes in the space group P2_1/a with unit cell dimensions a=7.745(2), b=19.164(5), c=10.787(4), β=107.87(2)°. The resuhs of structural analyses show that the two compounds have the same characteristics: the tridentate ligand formed by condensation occupies three of the four equatorial positions of vanadium and the rest equatorial position is occupied by alkoxy group RO~-. As RO~-group also bridges the sixth coordinated position of each vanadium atom, it brings about the formation of the new type binuclear complexes of vanadium.     

ELECTRONIC STRUCTURE OF THE T*-TYPE SUPERCONDUCTORS (Bi0.5Sr1.5)(Y,Ce)2Cu2Oy STUDIED BY PHOTOELECTRON SPECTROSCOPY

The electronic structure of T^*-type compounds (Bi_0.5Sr_1.5)(Y_2-xCe_x)Cu₂O_y has been studied by X-ray photoelectron spectroscopy. From analysis of the results, it was found that cation deficiency in Ce⁴⁺ introduced holes to conduction planes in the T^* phase as in the p-type infinite layer compounds. Some Cu ions in the sample without cation-deficiency contained two-oxygen coordination, which resulted in the incompleteness of the CuO₂ sheets. Bi ions in the T^* phase cuprates take exact valence of 3_{+, Pb ions cannot replace them due to the too large an ionic radius of Pb²⁺/Pb⁴⁺.}     

基于空间域的空间光通信系统接收信标光斑图像平滑处理

本文首先对基于空间域的图像平滑处理滤波 (中值滤波和平均值滤波 )算法原理及误差进行了分析 ,同时对实测光斑进行了图像平滑处理 ,实验结果表明 :进行图像平滑处理后的原图像噪声被有效地抑制和消除 ,光强分布较为平滑。这表明图像平滑处理工作能有效减小系统误差 ,提高APT跟踪精度     

(Bi,Cd)Sr_2(Ln,Ce)_nCu_2O_y超导体及界面反应的光电子能谱研究

用光电子能谱研究了(Bi.Cd)Sr_2(Ln,Ce)_(?)Cu_2O_y的电子结构,以及其与铝之间的反应.芯能级结果表明:(Bi,Cd)Sr_2(Ln,Ce)_(?)Cu_2O_y系列中n=1,2和3三种材料的结果基本一致,并且类似其它超导材料中相同元素的芯能级结果.在(Bi,Cd)Sr_2(Ln,Ce)_(?)Cu_2O_y与铝的界面处,铝与(Bi,Cd)Sr_2(Ln,Ce)_(?)Cu_2O_y中的元素发生强烈反应,Bi—O,Sr—O和Cu—O键受到破坏,铜的价态从+2变为+1,并且同时伴随着超 关键词：     

RLG INS/GNSS极区组合导航方法

针对航空飞行器跨极区飞行,导航坐标系转换导致滤波器结构变化,进而影响导航精度的问题,提出了基于协方差变换的环形激光陀螺惯导/全球导航卫星系统算法(Ring Laser Gyroscope Inertial Navigation System/Global Navigation Satellite System,RLG INS/GNSS).通过建立地理坐标系、格网坐标系下系统误差状态及其协方差的转换关系,设计了具有全纬度适用性的组合导航滤波器,并通过跑车实验以及半实物仿真实验对算法的有效性进行了验证.实验结果表明,协方差变换算法可以有效解决导航坐标系转换导致的滤波不稳定问题,相较于无协方差变换,系统状态误差减小一个数量级.     

EDA在线阵CCD驱动电路设计教学中的应用

CCD(电荷藕合器件)是一种广泛应用的固体成像器件,在CCD应用中的关键问题之一是其驱动电路的设计.在本科生实验课程中开设的CCD驱动电路设计实验能帮助学生巩固所学的模拟电路和数字电路的知识,使学生在分析、设计和动手能力等方面得到提高,使实验教学和课堂教学得到结合.本文给出了在实验课程中采用EDA软件针对线阵CCD TCD2252D驱动电路的几种设计方案.     

常压下Hg系1201相超导铜氧化合物的合成

本首次报道常压下Ｈｇ系１２０１相超导铜氧化合物的制备，方法简便，制备样品质量较好，超导转变温度达９４Ｋ。作还进行一步讨论了１２０１相常压下制备的最佳成相条件及其物相的稳定性。     

三齿配体酰(氧)钒配合物的晶体结构研究——Ⅰ.双聚{1-(2,4-戊二酮-(3-硝基苯甲酰)-单腙-2-乙氧基合氧钒(Ⅳ)}和双聚{1-(2,4-戊二酮-(3-硝基苯甲酰)-单腙-2-甲氧基合氧钒(Ⅳ)的晶体结构

以二乙酰丙酮氧钒VO(Acac)_2与间硝基苯甲酰肼m-NO_2PhCONHNH_2分别在乙醇和甲醇中反应,得[VO(C_(12)H_(12)N_3O_4)(C_2H_5O)]_2(Ⅰ)和[VO(C_(12)H_(12)N_3O_4)(CH_3O)]_2(Ⅱ)两种晶体。晶体(Ⅰ)属空间群P(?),晶胞参数a=8.123(2),b=10.409(5),c=10.822(4),α=65.78(3)°,β=85.50(3)°,r=89.04(3)°。晶体(Ⅱ)属空间群P2_1/a,a=7.745(2),b=19.164(5),c=10.787(4),β=107.87(2)°。两个晶体均具有共同的结构特征:通过缩合形成的三齿配体占据四个赤道配位位置中的三个,男一个赤道配位位置由醇氧基RO~-所补充而RO~-中的氧原子又兼作桥氧向另一个钒原子的第六位配位,从而导致文献中未报道过的新型双核钒配合物的形成。     

ELECTRONIC STRUCTURE OF THE T*-TYPE SUPERCONDUCTORS (Bi0.5Sr1.5)(Y, Ce)2Cu2Oy STUDIED BY PHOTOELECTRON SPECTROSCOPY

The electronic structure of T^*-type compounds (Bi_0.5Sr_1.5)(Y_2-xCe_x)Cu₂O_y has been studied by X-ray photoelectron spectroscopy. From analysis of the results, it was found that cation deficiency in Ce⁴⁺ introduced holes to conduction planes in the T^* phase as in the p-type infinite layer compounds. Some Cu ions in the sample without cation-deficiency contained two-oxygen coordination, which resulted in the incompleteness of the CuO₂ sheets. Bi ions in the T^* phase cuprates take exact valence of 3_{+, Pb ions cannot replace them due to the too large an ionic radius of Pb²⁺/Pb⁴⁺.}