首页> 外文期刊>Journal of Low Temperature Physics >The Effect of Gd Concentration on the Physical and Magnetic Properties of Bi_(1.7)Pb_(0.3-x)Gd_(x)Sr_(2)Ca_(3)Cu_(4)O_(12+y) Superconductors
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The Effect of Gd Concentration on the Physical and Magnetic Properties of Bi_(1.7)Pb_(0.3-x)Gd_(x)Sr_(2)Ca_(3)Cu_(4)O_(12+y) Superconductors

机译:Gd浓度对Bi_(1.7)Pb_(0.3-x)Gd_(x)Sr_(2)Ca_(3)Cu_(4)O_(12 + y)超导体的物理和磁性能的影响

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摘要

Bi-Pb-Gd-Sr-Ca-Cu-O bulk samples with nominal composition Bi_(1.7)Pb_(0.3-x)Gd_(x)Sr_(2)Ca_(3)Cu_(4)O_(12+y) (x velence 0.01, 0.05, 0.075, 0.10) were prepared by the melt-quenching method. The effects of different Gd doping on the structure have been investigated by electrical resistance, scanning electron micrographs, XRD, magnetization and magnetic hysteresis loop measurements. The magnetization measurements have been carried out as a function of magnetic field for fields up to 5 kOe at temperatures well below the zero resistance temperatures of the annealed samples. It has been found that the high-T_(c) superconducting phase, (2223), is formed in the sample A with concentration x velence 0.01, annealed at 840 deg C for 120 h. However, with increasing Gd~(3+) doping for Pb~(2+) the (2223) phase gradually transforms into the (2212) phase. The magnitudes of magnetization and initial susceptibility, |M| and |dM/dH|, and the hysteresis loop areas decrease with increasing Gd concentration x and/or temperature T. The fast decreases in |M|, |dM/dH|, and the hysteresis loop areas related to the superconducting volume, with increasing x and/or T seem to imply an existence of flux pinning centres in our samples. In order to support this implication the critical current densities J_(c), of the samples, have been estimated at two fixed temperatures, 9 and 30 K. Our data have indicated that J_(c) decreases with increasing temperature and/or Gd concentration, as expected.
机译:标称成分为Bi_(1.7)Pb_(0.3-x)Gd_(x)Sr_(2)Ca_(3)Cu_(4)O_(12 + y)的Bi-Pb-Gd-Sr-Ca-Cu-O块状样品通过熔融淬火法制备(x velence 0.01、0.05、0.075、0.10)。通过电阻,扫描电子显微图,XRD,磁化和磁滞回线测量,研究了不同Gd掺杂对结构的影响。在远低于退火样品零电阻温度的温度下,对于磁场高达5 kOe的磁场,已根据磁场进行了测量。已发现在样品A中形成高T_(c)超导相(2223),其浓度x速率为0.01,并在840摄氏度下退火120小时。但是,随着对Pb〜(2+)的Gd〜(3+)掺杂增加,(2223)相逐渐转变为(2212)相。磁化强度和初始磁化率| M |和| dM / dH |,并且磁滞回线面积随Gd浓度x和/或温度T的增加而减小。| M |,| dM / dH |的快速减小以及与超导体积有关的磁滞回线面积随x和/或T的增加似乎暗示我们样本中存在磁通钉扎中心。为了支持这种含义,已在两个固定温度(9和30 K)下估算了样品的临界电流密度J_(c)。我们的数据表明,J_(c)随着温度和/或Gd浓度的增加而降低,正如预期的那样。

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