109 resultados para Y-Ba-Nb-Cu-O


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滇东南地区北西以弥勒-师宗断裂与扬子地块分界,南西以红河断裂为界与哀牢山断块毗邻,南连越北古陆,东部文麻断裂与南岭褶皱系连为一体,是我国重要的锡、银、铅、锌等矿产基地,自西向东分布着个旧、白牛厂和都龙三个超大型银锡多金属矿床,在这三个大型矿床附近各分布着一个大花岗岩体,个旧和老君山岩体已有相当多的研究,而对于薄竹山岩体、薄竹山岩体接触带周边矿床和与临近白牛厂矿床的研究则相对薄弱。本文主要对薄竹山岩体进行岩石学、地球化学研究,并且借助铅同位素,对薄竹山岩体接触带矿床和白牛厂矿床的成矿物质来源作了分析,阐明这些矿床的形成与薄竹山花岗岩体的关系。 薄竹山花岗岩体分两期侵入,第一期岩石类型主要为中粒黑云母二长花岗岩,属于过铝质花岗岩,主要形成于同碰撞阶段;第二期主要为细粒二长花岗岩,形成于板内的伸展环境。与第一期相比,第二期花岗岩更加富硅富碱、贫钙贫镁,稀土配分曲线显示Eu亏损更加强烈,更加富集Rb、Ta、Tb、Y,而亏损Ba、Sr、La、Ce等元素。Sr-Nd同位素显示,两期花岗岩可能分别来源于中元古界地壳和太古宙古老基底。 薄竹山岩体长石铅同位素组成均一,其接触带矿床矿石铅与岩体长石铅分布趋势一致,所以接触带矿石铅可能主要由薄竹山岩体提供。对于白牛厂矿床,除个别样品外,矿区内西北白羊矿段和东南部其他矿段矿石铅组成一致,说明整个白牛厂矿区的矿石铅来源比较单一,并且与薄竹山附近矿化点矿石具有相似的铅同位素分布范围,说明两种矿石铅来源可能相同,都来源于薄竹山花岗岩浆。白牛厂矿区内赋矿地层铅与矿石铅同位素演化趋势完全不同,所以赋矿地层不可能为矿石铅的重要来源。 综合薄竹山岩体及矿石的铅同位素组成特征,我们发现白牛厂矿区内矿石铅主要来自薄竹山岩体,主要为矿区内隐伏岩体提供。白牛厂矿床早期可能发生过喷流沉积作用,但没有带来大量银、铅、锌等成矿物质,后来燕山期花岗岩浆侵入,带来大量银、铅、锌等成矿物质,形成了现在的白牛厂矿床。

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本文合成了 Ba_2P_(rx)Ln_(1-x)Cu_3O_(7-δ)系列化合物,测量了它们的超导电性(Tc),当 x=0.1,T_c(L_n=Y)=78.5K,T_c(Yd)=88K、T_c(Nd)<77K。晶胞参数及正交畸变与组成的变化图表明稀土元素的离子半径影响显著,讨论了 Ba_2LnCu_3O(7-δ)体系中 Cu-O 链、Cu-O 层及 Cu~(3+)对超导电性的作用,当 Ln 的价态界于三、四价之间时(如Pr),四价的成份越多,Cu~(3+)的量就越少,虽然正交畸变很大,但 T_c 降低。

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本文合成了LnBa_2Cu_(3(1-x))Ag_xO_(7-δ) (x = 0.1,0.3,0.5, Cu = Y,Dy,Ho,Er,Gd) YBa_(2(1-x))Cu_3Ag_xO_(7-δ) (x = 0.05,0.1,0.2,0.3,0.4,0.5,0.6); Y_(1-x)Ag_xBa_2Cu_3O_(7-δ) (x = 0.05,0.1,0.2,0.3,0.5); YBa_2Cu_3O_(7-δ)Ag_x (x = 0.2~2.0), CuBaCu_3O_(7-δ)Ag_x (x = 0.5,1.0, Cu = Dy,Ho,Er)及与之对照的空白样品等一系列超导稀土复合氧化物,对它们的结构、电学性质、Ag的存在状态及Ag的加入方式进行了研究。对这方面的研究目前仍无全面系统的报道。对CuBa_2Cu_(3(1-x))Ag_xO_(7-δ)的研究表明Ag并未取代Cu的格位,少量的Ag加入(x<0.1)就使结构发生破坏,当x>0.1时样品即失去超导性,对光加Ag的YBa_(2(1-x))Cu_3Ag_(2x)Cu_3O_(7-δ)的研究表明,当x<0.6时仍为90k左右的超导体,Ag没有取代Ba的格位,Ag的加入使杂相比例加大,Ag的加入改善了样品晶粒间的弱连接状况,使电流密度明显提高,Ag以单质及复合物形式存在于样品之中。后加Ag方式对结构、电性、无影响没有提高Jc。对光加Ag的Y_(1-x)Ag_xBa_2Cu_3O_(7-δ)的研究表明,x<0.5时样品仍为90k左右超导体,Ag的加入使杂相比例减少,Ag部分以单质及与13a、Cu形成对改善弱连接状有益的复合场的形式存在,部分进入晶格可能占据了Y的格位使C轴变长。Ag的加入改善了样品晶粒间的弱连接状况,从而使Jc大幅度提高,当x=0.1时Jc = 362 A/cm~2,后加Ag的方式对结构、电性、无影响没有提高Jc。对YBa_2Cu_3O_(7-δ)Ag_x的研究表明,加Ag的样品的Jc比不加Ag样品的Jc明显加大,随着Ag量的加大Jc增加,当x=1时Jc最大,当Ag量大于2.0mol时将有大量Ag析出,Ag的加入不影响超导正交结构,部分Ag进入了晶格可能占据了Y的格位,C轴增长,部分以单质及复合物的形式存在,Ag的加入不影响样品的临界温度,使样品电阻降低,电镜分析表明,Ag的加入改善了样品晶粒间的连接状况。CuBaCu_3O_(7-δ)Ag_x与上面体子有相同的性质,在加入1mol Ag得到,Jc:DyBaCu_3O_(7-δ)Ag_(1.0) 113A/cm~2;HoBaCu_3O_(7-δ)Ag_(1.0) 164 A/cm~2 ErBaCu_3O_(7-δ)Ag_(1.0) 177A/cm~2的样品。样品加Ag后密度明显加大,最大可达6.321克/cm~3,硬度也加大具有良好的机械性能。针对在YBaCu_3O_(7-δ)样品中添加Ag,可以做为一种大幅度提高Jc的途径的特点,进行了各种工艺探索,到目前为止,合成出了临界电流密度为570 A/cm~2的样品。

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The valences of Cu and bond covalencies in Y1-xCaxBa2Cu3O6+y, have been investigated using complex chemical bond theory, This theory is the generalization of Phillips, Van Vechten, Levine, and Tanaka's scheme. The results indicate that the valences of Cu(1) and Cu(2) in our calculation agree well with those obtained by the bond valence sum method. The valences of Cu(1) and Cu(2) in our calculation also suggest that the holes introduced by Ca substitution only reside in CuO2 planes and there is a competing mechanism for the hole density in CuO2 planes between,Ca doping and oxygen depletion. These conclusions are in satisfactory agreement with experiments. The calculated ordering of covalencies is Cu(1)-O(4)>Cu(1)-O(1)>Cu(2)-O(2,3)>Cu(2)-O(1)>Ca-O>Y-O similar to Ba-O, regardless of the Ca doping level and oxygen content. [S0163-1829(98)03325-6].

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The mixed oxides, including LaBa2Cu3O7, LaBaCu2O5, La4BaCu5O12 with perovskite structure, were prepared. The catalysts were characterized by means of chemical analysis, XRD, H-2-TPR. It was found that their structures were layered ABO(3) perovskite structure and they were the active catalysts for the NO reduction by CO. The existence of Cu3+ is an important factor to give the catalysts a high activity for the NO reduction by CO.

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The mixed oxides, including YBa2Cu3O7, LaBa2Cu3O7, LaBaCu2O5, La2BaCu3O7, La4BaCu5O12 with perovskite structure, were prepared. The catalysts were characterized by means of chemical analysis, XRD, TPD and TPR method. It was found that they were the active catalysts for the NO decomposition and NO reduction by CO. The existance of Cu3+ is an important factor to give the catalysts a high activity for the NO reduction by CO.

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稀土元素成矿与地壳的构造运动密切相关,稀土在中元古代具有大规模暴发性成矿特征。云南武定迤纳厂稀土铁铜矿床为昆阳群因民组出现稀土富集成矿的典型代表。本论文选择迤纳厂矿床为主要研究对象,系统研究矿床不同类型岩(矿)石和矿物的稀土元素地球化学特征,探讨富稀土的成矿流体、成矿物质来源和稀土元素成矿时代,揭示昆阳裂谷初期因民组稀土元素富集的地球化学机制。主要认识如下:1、迤纳厂矿床产于昆阳裂谷初期形成的禄丰一武定火山断陷盆地中。早中元古界昆阳群分布于绿汁江岩石圈断裂和小江一易门断裂的夹持地带,呈狭长状展布。迤纳厂矿床赋矿地层为昆阳群因民组上段的硅质白云岩和碱性火山岩(粗面安山岩)。矿体产出形态和矿石的结构构造等均显示矿体与赋矿地层同沉积特征;出现独立矿物氟碳饰矿、独居石及褐帘石,磷灰石、萤石、菱铁矿等矿物中也含有一定量的稀土,沿矿体走向和垂向稀土元素变化不大。2、矿体顶、底板围岩(石榴石黑云母片岩、钠长黑云母片岩等)的原岩为碱性火山岩(粗面安山岩),相对富集大离子亲石元素Ba、Cs、Rb、K、LRE日及贫Zr、Sr、Ti、Hf、HEE,为早元古代末期一中元古代早期交代富集地慢低程度部分熔融所形成的碱性火山岩。矿石稀土总量高(645-4443)×10-6,强烈富集轻稀土((La/Tb)N=17.3-81.1),稀土元素分布特征明显不同于矿区正常沉积的硅质白云岩和后期侵入的钠长石英斑岩及火山角砾岩,而与矿体顶、底板碱性火山岩中稀土元素配分特征基本一致,暗示稀土成矿物质来源与碱性火山岩有密切的关系;3、矿石中微量元素组合及变化特征与现代海底正在喷出的热液和热液沉积物中元素组合有较大的可比性,明显不同与火成碳酸岩型稀土矿床中的特征元素组合;在微量元素判别图解(Al-Fe-Mn、Fe/Ti-Al/(Al+Fe+Mn)、U-Th、Y-P2O5等)中,逸纳厂矿石均投影在热水沉积区,矿石的Y/Ho值与黑烟囱值接近,表明成矿流体为高温、还原性质,稀土成矿可能以热水沉积作用方式为主;4、对矿石中主要矿物萤石、菱铁矿、磁铁矿、石英、方解石的稀土元素特征研究表明,矿石沉积时不同矿物中稀土元素分布特征基本相同,主要受成矿流体中稀土分布特征制约。而后期变质作用形成的矿物,其稀土元素分布主要受矿物晶体结构控制。同期成矿流体从早期到晚期(块状矿石→条带状矿石),轻重稀土分异变小,稀土总量增加,条带状矿石中稀土含量最高;矿石黄铜矿6345值变化在一任3%0到2g%。范围,显示慢源硫特征;菱铁矿6r3C(8%-9.1%)、δ18O(-11.17%-15.37)‰指示成矿流体具岩浆来源和有机质的脱梭酸分解作用参与;成矿流体中稀土元素可能主要以(RE(CO3)3F)4-、(既(CO3)3F2)、(RE(F,Cl万等形式迁移,当温度降低时沉淀出氟碳饰矿等稀土矿物;5、矿石和萤石单矿物 Sm-Nd等时线年龄分别为1621士110Ma和15:38士43Ma,与矿区碱性火山岩错石的U-Pb年龄1676Ma、因民组顶部石英正长斑岩的错石U-P1。年龄1685Ma基本一致,也与因民组地层年龄1765M。较为接近,反映成矿时代为早元古代晚期和中元古代早期:这一时间也与一早元古代晚期一中元古代早期昆阳裂谷初始裂陷阶段,大量来自于地幔的碱性火山岩喷发事件相吻合。矿石。Nd(t):-2.87-3.60,萤石单矿物εNd(t):-3.93-5.90,变化范围较窄并全为负值,接近0,指示源区为富集地幔。同时结合矿床形成的构造一地质环境及矿体产出的地质形态,认为逛纳厂稀土铁铜矿床可能是在昆阳裂谷初期,在碱性火山岩浆喷发的间歇期,来自地幔富稀土、挥发份的成矿流体由火山喷流一同生沉积方式形成的矿床。6、昆阳群因民组地层中出现的稀土富集、成矿与我国的白云鄂博稀土REE-Fe-Nb超大型矿一床和澳大利亚的olympic Dam Cu-U-Au-Ag-REE超大型矿床,在成矿时代、产出大地构造背景、成矿物质来源等方面具有较大的相似性,均体现成矿受控于中元古代1.5Ga超大陆聚合前或随后裂解初始阶段伴随的非造山型碱性岩浆或热液作用,稀土来源于超大陆拼合前因板块俯冲交代而形成的富集地幔。

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(Zr65Al10Ni10Cu15)(100-x) Nb-x glass forming alloys with Nb contents ranging from 0 to 15 at.% were prepared by water-cooled copper mould cast. The alloys with different Nb contents exhibited different microstructures and mechanical properties. Unlike the monolithic Zr65Al10Ni10Cu15 bulk metallic glass, only a few primary bee beta-Ti phase dendrites were found to distribute in the glassy matrix of the alloys with x = 5. For alloys with x = 10, more beta-phase dendrites forms, together with quasicrystalline particles densely distributed in the matrix of the alloys. For alloys with x = 15, the microstructure of the alloy is dominated by a high density of fully developed P-phase dendrites and the volume fraction of quasicrystalline particles significantly decreases. Room temperature compression tests showed that the alloys with x = 5 failed at 1793 MPa and exhibited an obvious plastic strain of 3.05%, while the other samples all failed in a brittle manner. The ultimate fracture strengths are 1793, 1975 and 1572 MPa for the alloys with x = 0, 10 and 15 at.% Nb, respectively.

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对于稀土与非稀土所组成的二元复合氧化物的研究国外已有较多的报导。但是,对于稀土和锑的复合氧化物只是近年来才开始有些研究工作。含锑与稀土的多元复合氧化物的报导就更少。本文在我们实验室张静筠等人三元复合氧化物研究的基础上,开展Mo—Sb_2O_5—R_2O_3—R'_2O_3—Bi_2O_3多元体系的研究工作,这对于我国丰产元素稀土和锑的应用以及利用Bi~(3+)的激活与敏化将是有益的。本文按Thornton等人的方法合成了Ba_2BiSbO_6,Ba_2GdSbO_6,按EγΦECEHKO等人的方法合成了M_2RSbO_6 (M = Ba、Sr、Ca, R = La Y)。并以M_2RSbO_6为基质,掺Sm~(3+)、Eu~(3+)、Dy~(3+)、Ho~(3+)、Er~(3+)、Tm~(3+)和Bi~(3+),研究它们的化学组成,晶体结构与发光性能的关系及规律,Bi~(3+)的荧光和敏作用。同时研究了它们的磁学和热学性能。化学组成的分析结果表明,计算的含量与实验测得的含量符合较好,说明化学反应是按化学计量比进行的。通过X-射线粉沫物相分析和晶胞参数的理论计算确定M_2RSbO_6(M = Ba、Sr、R = La、Y、Gd、Bi)复合氧化物是属于立方钙钛太型化合物。空间群为Fm3m,点群为Oh。用计算机计算了Ca_2YSbO_6的晶胞参数并结合荧光光谱分析确定它属于畸变的单斜钙钛矿,空间群为P_(21)。用磁天平测量了样品M_2RSbO_6 (M = Ba、Sr、Ca; R = Gd、Y、Bi)的磁化率。除Ba_2GdSbO_6是顺磁性物质外共余的都是反磁性的物质。按所用原料Sb_2O_5计算的磁化率与测量值符合较好,表明在所研究的M_2RSbO_6化合物中锑是正五价的。用热重热差分析仪测量了样品在反应中的热性能,观察到在化合物形成的过程中所用原料Sb_2O_3大约在520 ℃左右氧化变为Sb_2O_5。除所用原料碳酸盐分解外没有挥发性的物质,这就进一步证明化学组成分析和磁化率测量的结果是正确的。光学测量的结果表明,所有的磷光体随着激活离子浓度的不同其光谱都发生规律性的变化。对于不同Eu~(3+)浓度的Ba_2YSbO_6:Eu~(3+)和Br_2YSbO_6:Eu~(3+), Bi~(3+)体系用254nm激发时均能观察到Eu~(3+)于595nm的尖峰发射。用基质和Bi~(3+)的激发峰325nm激发时,明显地看到敏化剂Bi~(3+)到Eu~(3+)的能量传递,使Eu~(3+)于595nm的发射大大增强,我们认为Bi~(3+)对Eu~(3+)的敏化作用是由于基质和Bi~(3+)的~1S。→ 3P_1的跃迁吸收了激发的能量,然后无辐射弛豫到Eu~(3+)的激发态~5D_0,产生~5D_0 → 7F_1的磁偶极跃迁。对于不同Eu~(3+)浓度的Sr_2YSbO_6:Eu~(3+)和Sr_2YSbO_6:Eu~(3+), Bi~(3+)体系用245nm激发时均能观察到Eu~(3+)于595nm的尖峰发射。用基质和Bi~(3+)的激发峰335nm激发时,观察到基质和Bi~(3+)对Eu~(3+)具有某种能量传递。敏化作用机理与上述的Ba_2YSbO_6:Eu~(3+)和Ba_2YSbO_6:Eu~(3+), Bi~(3+)体系相同。对于不同Eu~(3+)浓度的Ca_2YSbO_6:Eu~(3+)和Ca_2YSbO_6:Eu~(3+), Bi~(3+)体系用396nm激发时,均能观察到Eu~(3+)于613nm很强的尖峰发射。用基质和Bi~(3+)的激发峰313nm激发时,见到Bi~(3+)和基质对Eu~(3+)具有某种能量传递,这种敏化作用主要是由于基质和Bi~(3+)的3P_1 → ~1S_0的400nm的宽带发射和Eu~(3+)的~7F_0 → ~5L_6的396nm的吸收相匹配产生~5L_6→~5D_0→~7F_2的跃迁。通过对激发光谱和荧光光谱的分析给出了Ca_2Y_(0.96)Eu_(0.04)SbO_6的能级图,从实验上可见,Eu~(3+)的发光强烈地依赖于钙钛矿的结构,当Eu~(3+)在空间群为Fm3m 的Ba_2YSbO_6和Sr_2YSbO_6中处于Oh点对称性时,主要是~5D_0 → ~7F_1的磁偶极跃迁。当Eu~(3+)在空间群为P_(21)的单斜钙钛矿中时,主要是~5D_0 → ~7F_2的电偶极跃迁。对于不同掺杂浓度M_2YSbO_6:R~(13+)(M = Ba、Ca; R' = Sm、Dy、Ho、Er、Tm)体系,通过激发和荧光光谱的研究,合理地确定了谱项。发现基质对Sm~(3+)、Dy~(3+)、Ho~(3+)具有敏化作用。对不同Bi~(3+)浓度的Ca_2YSbO_6:Bi~(3+),由激发和荧光光谱可见Bi~(3+)具有二个激发带,第一激发带位于240nm处相当于~1S_0 → ~1P_1的跃迁,第二激发带位于315nm处相当于~1S_0 → ~3P_1的跃迁。有一个很强的兰紫色发射位于400nm处相当于~3P_1 →~1S_0的跃迁。

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本文合成了LaBa_2Cu_(3-x)Sn_xO_(6.5) + x (x = 0.2; 0.5; 0.7; 1.0; 1.2; 1.5; 1.7; 2.0; 2.2; 2.5; 2.7; 3.0)系列,2aBaCu_(2-x)Sn_xO_(4.5) + x (x = 0; 0.2; 0.5; 0.7; 1.0; 1.2; 1.5; 1.7; 2.0)系列和La_3Cu_(3-x)Sn_xO_(7.5) + x (x = 0.5; 1.0; 1.5; 2.0; 2.2; 2.5; 2.7)系列等二十八个新复合氧化物。这三个系列二十八个新复合氧化物直至目前为止,文献上未见过报道。我们通过x-ray粉末衍射图分析了它们的结构,肯定了它们是新的单一化合物,计算了它们的晶胞参数并确定它们的所属晶系。元素化学分析表明,所有这些化合物均可用原始计算配比化学式表示。干湿两种合成方法所合成的结构相同。对于这三个系列二十八个瓣复合氧化物,我们选用LaBa_2-Cu_(3-x)Sn_xO_(6.5) = x (x = 0.5;1.0;1.5;2.0;2.5),LaBaCu_(2-x)Sn_xO_(4.5) = x(x = 0.5; 1.0; 1.5;2.0), La_3Cu_(3-x)Sn_xO_(7.5) + x (x = 0.5; 1.0; 1.5; 2.0; 2.5)等十四个化合物,对它们的低温,高温和高湿下的电阻率和导电类型进行了测试,绘得了它们的电阻率和温度的关系曲线。在一定温度下,一个系列内的化合物电阻率随锡的分子含量增加而增大。La_3Cu_(3-x)Sn_xO_(7.5) = x系统人物的电阻率明显大于其它二个系列相应化合物的电阻率。所有化合物在液氮至室温温区内,基本上呈半导体导电类型。在高温以上温区,当温度升至一定温度时之前,化合物呈本导体导电类型达到一定温度之后,当金属导电类型所有新复合氧化物在高温均属P型半导体。本文还研究了这三个系列化合物和将它们掺入二氧化锡中的气敏性能。结果表明:所有这类化合物和将它们掺入二氧化锡中作为添加剂做成的气敏材料,除LaBa_2Cu_(1.5)Sn_(1.5)O_8掺入SnO_2做成的气敏材料外,在本文实验条件下做成的气敏元件对氧化性和还原性气体均无或只有很差的气敏性。LaBa_2Cu_(1.5)Sn_(1.5)O_8作为添加剂掺入SnO_2中(摩尔比0.2:0.8; 0.1:0.9)所制得的气敏文件对高浓度(1%-10%)的一氧化碳,液化气和煤气具有很好的气敏线性响应,当加热电流为300mA时,酒精,汽油和石油醚等还原性气体基本上无干扰。实验表明当摩尔比为0.1:0.9时,材料的气敏性能最佳,但重现性较差,当摩尔比为0.2:0.8时,气敏性稍低,但重现性较好。本文还合成了La_xBa_(1-x)SnO_3(x = 0; 0.05; 0.10; 0.15, 0.20)系列化合物,并确定了它们的结构和所属晶系。从结构上分析我们认该系列化合物相互之间为置换固溶体。其晶胞参数随镧的加入量增加而减小。该系列均属几型半导体材料。我们利用该系列材料进行了过敏性研究。结果表明。由La_(0.1)Ba_(0.9)SnO_3制得的高热式气敏器件对低浓度酒精(<1000 ppm)有很好的气敏线性响应。在加热电流为250 mA时,基本上排除了煤气,一氧化碳,液化气和汽油等可燃性气体的干扰。但香烟烟雾对器件检测酒精有一定的影响。La_(0.1)Ba_(0.9)SnO_3气敏材料多添加1%而制得的器件,机械强度达到很好的效果,器件对酒精的灵敏度有降低,而响应浓度区间宽度增加近一倍,选择性几乎不变。该材料具有较好的实验重现性。该系列的其它化合物在本实验条件下所制得的器件对可燃性气体的敏感性较差。

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A series of complex perovskite solid solutions of Ba[(Mg1-xCdx)(0.33)Nb-0.67]O-3 have been synthesized by the columbite method. Detailed Rietveld refinement of their X-ray diffraction data show that Ba[(Mg1-xCdx)0(.33)Nb(0.67)]O-3 has an order trigonal structure. The ordering degree as determined by the B-site occupancies increases with the partial substitution of Cd for Mg.

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The valences of Cu in Y1-xGaxBa2Cu3O6+y have been investigated by using complex chemical bond theory The results for the valences of Cu(1) and Cu(2) in the calculation suggest that the holes introduced by calcium substitution only reside in CuO2 planes, and there is a competition mechanism for the hole density in CuO2 planes between Ca doping and oxygen depletion. These conclusions are satisfactorily in agreement with experiments.

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RBa2Cu3O7 (R = Pr, Sm, Eu, Gd, Dy, Y, Ho, Er, Tm) has been studied using complex chemical bond theory. The results indicated that with the decreasing of R radius, the ionicities for all considered types of bond decrease. This is in good agreement with the experimental fact that T-c decreases with the decreasing of R radius. PrBa2Cu3O7 with no Ba-site Pr in this calculation is also predicted to be a superconductor. This supports the conclusion obtained by Blackstead et al. The ionicity for each bond obeys the following order: Ba-O > R-O > Cu(2)-O(1) > Cu(2)-O(2,3) > Cu(1)-O(4) similar to Cu(1)-O(1).

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合成了具有钙钛石结构的复合氧化物YBa2Cu3O7、LaBa2Cu3O7、LaBaCu2O5、La2BaCu3O7和La4BaCu5O12.考察了它们对NO分解和NO+CO反应的催化性能.结合化学分析、XRD、TPD和TPR对催化剂的表征结果,探讨了该系列复合氧化物对NO分解和NO+CO反应的催化机理.

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With XRD, R-T, and ac chi measurements a comparative study on the doping effects of 3d elements in Bi(1.5)Pb(0.2)Sr(2)Ca(2)Cu(2.8)M(0.2)O(y) (M = Sc, Ti, V, Cr, Mn, Fe, Co, Ni, or Zn) has been carried out. The effects of the former five members are significantly different, both on phase formed and on T-c, from the latter four. It seems that the effect on phase stabilization correlates with the valency of the doped cation. In connection with the instability of the 2223 phase, the correlation has been discussed.