Y0.5Gd0.5Ba2Cu3O7-δ体系中通氧时间对超导转变温度的影响

研究了高温氧化物超导体Y0.5Gd0.5Ba2Cu3O7-δ体系中通氧时间对超导转变温度及超导转变温区的影响。Y0.5Gd0.5Ba2Cu3O7-δ样品是按相等摩尔数的Gd与Y元素配比,采用传统的固相反应法烧结而成的多晶块材。实验结果显示:Y0.5Gd0.5Ba2Cu3O7-δ烧结样品与YBa2Cu3O7-δ烧结样品均具有很好的单相性,在一定的通氧条件下其超导临界转变温度TC与超导初始转变温度TCO值相对YBa2Cu3O7-δ烧结样品有提高。文中对此结果进行了讨论。     

暂态热重法分析混合导电材料YBa_2Cu_3O_(7-δ)的透氧性能

用暂态热重法研究了 YBa2 Cu3O7-δ(YBCO)粉末在不同的温度下 N2 → O2 → N2 交变气流中的吸氧、脱氧过程 ,估算了其在不同温度下的氧吸附速率、氧脱附速率。结果表明 ,YBCO对氧有强烈的选择吸附性 ,并且其吸氧、脱氧过程是可逆的 ,氧吸附过程较迅速 ,而氧脱附过程则较缓慢 ;氧吸附或氧脱附过程在开始阶段是表面扩散 ,以后主要是体扩散。     

Y1-xRxBa2Cu3O7—δ体系（R=Eu、Gd）的正电子寿命和超导性研究

本文报道了对Y1-xRxBa2Cu3O7-δ（R=Eu、Gd）两个系列样品的超导电性研究结果．首先，发现随着Eu、Gd掺杂量x的增加，Y1-x]EuxBa2Cu3O7-δ和Y1-xGdxBa2Cu3O7-δ的晶胞体积均随之增大．但所有样品均保持与Y-123样品相同的单相正交结构；正电子平均寿命实验结果表明Cu—O链处局域电子密度ne随Eu、Gd掺杂浓度x的增加而减小．说明Eu、Gd对Y位的替代引起晶胞结构参量的变化不汉改变了Y位的电子密度．同时也影响了Cu-O链周围的电子密度分布；超导转变温度Tc随Eu、Gd掺杂浓度x增加而略有增加，反映了Eu、Gd掺杂虽然改变了体系的局域电子结构．但没有破坏超导所需的Cu-O链与CuO2面之间的耦合：Y位掺杂体系的超导电性与掺杂离子的磁性无关，而与掺杂离子的半径有关．     

Y1-xRxBa2Cu3O7-δ体系R=Eu、Gd)的正电子寿命和超导性研究

本文报道了对Y1-xRxBa2Cu3O7-δ(R=Eu、Gd)两个系列样品的超导电性研究结果.首先,发现随着Eu、Gd掺杂量x的增加,Y1-x〗EuxBa2Cu3O7-δ和Y1-xGdxBa2Cu3O7-δ的晶胞体积均随之增大,但所有样品均保持与Y-123样品相同的单相正交结构;正电子平均寿命实验结果表明Cu-O链处局域电子密度ne随Eu、Gd掺杂浓度x的增加而减小,说明Eu、Gd对Y位的替代引起晶胞结构参量的变化不仅改变了Y位的电子密度,同时也影响了Cu-O链周围的电子密度分布;超导转变温度T\-c随Eu、Gd掺杂浓度x增加而略有增加,反映了Eu、Gd掺杂虽然改变了体系的局域电子结构,但没有破坏超导所需的Cu-O链与CuO2面之间的耦合;Y位掺杂体系的超导电性与掺杂离子的磁性无关,而与掺杂离子的半径有关.     

Y(Ba_(1-x)Gd_x)_2Cu_3O_(7-δ)的临界电流密度特征

多晶样品Y(Ba1-xGdx)2Cu3O7-δ(YBGCO)(x=0.0,0.02,0.03,0.05,0.08,0.10)是由标准固相反应法制备获得。XRD的Rietveld精修显示,Gd成功地部分替代YBa2Cu3O7-δ(YBCO)晶胞中的Ba位。实验结果表明,对于某一固定磁场Y(Ba1-xGdx)2Cu3O7-δ的临界电流密度(Jc)在x=0.05有最大值。此外,尽管YBGCO的超导温度(Tc)明显地单调下降,但微量的Gd掺杂导致磁场中YBGCO的Jc的提高。Jc随着Gd掺杂量不同而变化的特征行为可以认为,是由Gd掺杂引起的两种不同的效果竞争共同作用造成的,即纳米尺度范围内空间分布不均匀性和超导性的变化。     

钙钛矿型氧载体SrCo_(0.8)Fe_(0.2)O_(3-δ)制氧性能的实验研究

钙钛矿型金属氧化物是优良的制备供富氧燃烧所需的O_2/CO_2的氧载体,本文采用柠檬酸法制备系列SrCo_(1-x)Fe_xO_(3-δ)(x=0.2,0.4,0.6,0.8)钙钛矿型氧化物,并采用X射线衍射分析来表征SrCo_(0.8)Fe_(0.2)O_(3-δ)(SCF182)反应前后的物相变化和晶体结构.同时在固定床上选择不同的运行条件对SCF182的释氧性能进行研究,包括吸附温度、吸附时间、脱附温度和循环特性.结果表明,SCF182的最佳吸附温度和脱附温度均为850℃,最佳吸附时间为1 h,循环性能良好,是可以为富氧燃烧提供稳定的O_2/CO_2循环气体的良好材料。     

Co掺杂的YBa2Cu2O6+δ的氧非计量和氧渗透性能研究

研究钴离子部分取代铜离子对YBa2 Cu3 O6+δ的氧非计量值δ和氧渗透率的影响 .对于钴替代的样品 ,氧非计量的绝对值变大 ,且其数值不再随温度和氧分压的变化发生显著变化 .YBa2 Cu2 CoO6+δ样品在中、高温具有可观的氧渗透率 .对于厚度为 1.2mm的致密YBa2 Cu2 CoO6+δ样品 ,在 85 0℃时 ,只要在样品两端施加较小的氧分压差(PO2 =2 1.2kPa、PO2 =10 1Pa) ,其氧渗透率即可达 5 7μmol/cm2 s,明显高于YBa2 Cu3 O6+δ的氧渗透率 (31μmol/cm2s) .YBa2 Cu2 CoO6+δ的高氧渗透率在结构上可被归结为位于晶胞基面上的氧离子和氧空位的均匀分布     

高温超导体Y1-xCaxBa2Cu3O7-δ和Y-123/Cax体系的超导输运特性研究

本系统地研究了Y-123高温超导体Ca掺杂样品Y1-xCaxBa2Cu3O7-δ(x=0,0．1,0．2,0.3)和Y-123／Cax(x=0．1,0．2,0．3)样品的超导特性,对样品的临界温度Tc及输运特性进行了对比分析．实验发现：随着Ca含量增加两组样品的Tc有不同程度的递减,样品Y1-xCaxBa2Cu3O7-δ的Tc随Ca含量增加的变化规律正好与样品Y-123／Cax相反．Ca元素的加入使两组样品临界电流都有明显提高,但在Y-123／Ca,中表现得更为明显,并且受磁场的影响更小．实验中还发现,Y1-xCaxBa2Cu3O7-δ的I-V曲线存在负磁阻区,而在Y-123／Cax中却没有发现．     

Y_2O_3和BaCeO_3掺杂对YBa_2Cu_3O_(7-δ)多晶结构和超性质的影响（英文）

本文采用固相反应方法制备了一系列YBa2Cu3O7-δ(Y123)+0.25molY2O3+x wt%BaCeO3(x=0.0,2.0,5.0,10.0and 20.0)多晶样品,通过X射线衍射法(XRD)和扫描电子显微镜(SEM)对Y2O3和BaCeO3的参杂的样品微观结构和超导转变温度进行系统的测量,发现Y2O3参杂到YBCO样品表面有球形或椭球形Y2Ba1Cu1O7-δ(Y211)粒子形成.依据SEM,XRD和电阻率测量,随着BaCeO3参杂量的增加,我们观察到样品的形貌变得越来越不均匀,所有样品的晶体结构有从正交相向四方相转变的趋势,超导转变温度呈金属状态到半导体状态转变的趋势,并伴有三步转变过程;同时也观察到了超导转变温度降低且转变宽度增加的现象,这些结果可以用氧分布的变化和缺陷的变化及氧缺陷来解释.     

Co掺杂对YBa_2Cu_3O_(7-δ)电阻率与塞贝克系数的影响

用固态反应法制备了YBa2Cu3-xCoxO7-δ(x=0.0,0.1,0.2,0.5)样品,研究了Co掺杂对YBa2Cu3O7-δ高温区的电阻率和塞贝克系数的影响。随着Co含量的增加,样品的电阻率和塞贝克系数逐渐增大,从金属性导电转变为p型半导体导电。x=0.2和0.5样品的电导活化能在500K处发生突变,高温区的活化能大于低温区的活化能。通过塞贝克系数与温度的关系,计算出x=0.2和0.5样品的费米能级分别为0.02和0.12 eV。当温度高于650-700K时,氧脱附显著影响样品的电输运性质,导致电阻率和塞贝克系数随温度增加而增大。     

掺Ce的Y－Ba－Cu－O体系成相的拉曼光谱分析

掺Ｃｅ的Ｙ－Ｂａ－Ｃｕ－Ｏ体系成相的拉曼光谱分析许存义，左健，王跃（中国科学技术大学结构分析开放研究实验室合肥２３００２６）ＳｔｕｄｙｏｎＴｈｅＲａｍａｎＳｐｅｃｔｒｕｍｏｆＣｅ－ｄｏｐｅｄＹ－Ｂａ－Ｃｕ－ＯＳｙｓｔｅｍ￥ＣｕｎｙｉＸｕ；ＪｉａｎＺｕ...     

Co掺杂对YBa2Cu3O7-δ微观结构及透氧性能的影响

利用XRD、TG和标准四电极法研究了YBa2Cu3-xCoxO7-δ(x=0~0.5)混合导体的结构和性能,稳态法考察了Co掺杂量对膜材料透氧性能的影响。实验表明当x<0.05时,Co掺杂可以提高透氧量,在x=0.05时达到最大值(940℃,厚1.4mm的膜材料透氧量为0.53ml/min.cm2)。当x>0.05透氧量开始减小,当x>0.01后,透氧量下降到比未掺杂的YBa2Cu3O7-δ还要小。从晶格结构与Co掺杂量的关系及Co-O键能与Cu-O键能的差别对透氧量随Co掺杂量的变化进行了讨论。     

Laser scattering,transmittance and low thermal expansion behaviors in Y_(2-x)(ZnLi)_xMo_3O_(12) by forming regular grains

Ceramics usually have irregular grains, cracking, or porosity, which result in their lightproof.Y_2Mo_3O_(12) ceramics have more porosity due to the heavy hygroscopicity.Introducing ZnLi to Y_2Mo_3O_(12) could form regular grains, reduce cracking and porosity.With increasing the content of ZnLi, the grain shapes self-assembly gradually and then the laser scattering and transmittance improve.The laser scattering property and transmittance of diverging rays become the best in ceramics Y_(2-x)(ZnLi)_xMo_3O_(12)(x = 1.0 and 1.2) with regular grains and low thermal expansion.The formation mechanism of regular grains is ascribed to the substitutions of Zn~(2+)and Li+for Y~(3+) in Y_2Mo_3O_(12) resulting in the preferential growth.The investigation in laser scattering, transmittance and low thermal expansion behaviors of Y_(2-x)(ZnLi)_xMo_3O_(12) could pave a way to weaken the strong-laser attack from the high-power laser weapon and the other.     

Combinative energy, oxygen deficiency and superconductivity in LnBa2Cu3O7-x （Ln=Nd, Er, Sm）

The correlation among the combinative energy, superconductivity, oxygen content, the position of holes in different planes, and the position of holes in the Cu(2)-O plane in LnBa2Cu3O7-x (Ln=Nd, Er, and Sin) has been investigated on the basis of a block model. The results indicate that the combinative energy decreases with increasing Tc in all of these compounds. And also, the combinative energies are obviously different with holes at different positions in the Cu(2)-O plane when the oxygen deficiency is low. However, this difference becomes less with increasing the oxygen deficiency.The effect of the holes in different positions on the combinative energy supplies some clue to the understanding of an unresolved problem, i.e. whether the distribution of carriers in the CuO2 plane is uniform or inhomogeneous. The results not only show that the structural characters, the combinative energy between two structural blocks and the superconductivity are closely interrelated in this class of compounds, but also reveal some differences among these systems. The relationship between the combinative energy and the Tc value in NdBa2Cu3O7-x shows some features different from the systems containing Er or Sm.     

高温超导体氧振模的混合

为解释高温超导晶体的声子Ｒａｍａｎ偏振谱，本文提出两个Ａ＿（ｌｇ）－对称声子模相混的机制。对Ｙ—Ｂａ—Ｃｕ—Ｏ单晶，按偏振Ｒａｍａｎ谱强度比计算了两个Ａ＿（ｌｇ）－振动模的耦合系数。     

Optical Response of Granular YBCO Weak Link

1.IntroductionRecently,thcrehasbecnintcrcstinthephot0resp0nse0fhigh-7'.oxidcsuperconductingfilms,espcciallywithregardtdthedctailsofthephysics0ftheph0toresponse['~'J.Fr0mtheviewpointoftheapplicationinthesuperconductingclectr0nics,thecharacteristicsofphotore-sponcse0fJosephsonjuncti0nfabricated\viththcsehigh-T.0xidcsupercondictorsandthepho-toinducedn0ncquilibriumproPerties0fthesematerialsmustbecxaminedandeva1uatcdforthedeve1opmcntofnQveIsL1pcrc0n(luctingdcviccsandJ0scphsoncbnjuncti0n.Itisf0un…     

Sr14-xCaxCu24O41的芯能级光电子发射谱

测量了准一维1/2自旋的反铁磁体系Sr14-xCaxCu24O41(x=0、3.5、6、7、8.4)多晶样品的芯能级光电子发射谱.各样品的Cu2p3/2的光电子发射谱中主峰峰位位于933.8eV左右,半高宽为3.3eV左右,拟合结果表明,当x=0时,Cu2+和Cu3+的质量分数分别为92.13%和7.87%;而Ca对A位Sr的替代对B位Cu芯能级的影响不明显,Cu2+和Cu3+的质量分数变化很小,估算得该体系中Cu离子的平均化合价为2.08;O1s的光电子发射谱中峰位位于531.0eV左右,并由于Ca对Sr的替代导致在低结合能方向出现一个小的台肩,该台肩来自于Ca-O键的贡献;Ca2p3/2的光电子发射谱中峰位位于346.4eV左右,Sr3d5/2的光电子发射谱中峰位位于133.4eV左右,证明在该体系中Ca和Sr的化合价均为+2价,没有混合价态存在.     

BaCuO_2的添加对YBa_2Cu_3O_(7-δ)临界电流密度的影响

掺入BaCuO2杂相的YBa2Cu3O7-δ(YBCO)粉末样品采用固相反应方法制备获得。XRD的Rietveld精修显示BaCuO2杂相和YBCO并存。在YBCO+xBaCuO2(x=0,0.05,0.1,0.2,0.3)的一系列样品中,当x=0.05时,样品的临界电流密度最大。在磁场中,微量BaCuO2杂相的添加,使YBCO的临界电流(Jc)提高了,但超导转变温度(Tc)稍微有所下降。临界电流密度的这些特征行为来自于两方面的共同作用,一方面是超导性的变化,另一方面纳米尺寸范围内的空间分布的非均匀性。     

Low-energy(40 keV) proton irradiation of YBa_2Cu_3O_(7-x) thin films:Micro-Raman characterization and electrical transport properties

To investigate the damage profiles of high-fluence low-energy proton irradiation on superconducting materials and related devices, Raman characterization and electrical transport measurement of 40-keV-proton irradiated YBa_2Cu_3O_(7-x)(YBCO) thin films are carried out. From micro-Raman spectroscopy and x-ray diffraction studies, the main component of proton-radiation-induced defects is found to be the partial transition of superconducting orthorhombic phase to the semiconducting tetragonal phase and non-superconducting secondary phase. The results indicate that the defects induced in the conducting CuO_2 planes, such as increased oxygen vacancies and interstitials, can result in an increase in the resistivity but a decrease in the transition temperature TCwith the increase in the fluence of proton irradiation, which is confirmed in the electrical transport measurements. Especially, zero-resistance temperature TC_0 is not observed at a fluence of 10~(15)p/cm~2.Furthermore, the variation of activation energy U_0 can be explained by the plastic-flux creep theory, which indicates that the plastic deformation and entanglement of vortices in a weakly pinned vortex liquid are caused by disorders of point-like defects. Point-like disorders are demonstrated to be the main contribution to the low-energy proton radiation damage in YBCO thin films. These disorders are likely to cause flux creep by thermally assisted flux flow, which may increase noise and reduce the precision of superconducting devices.