Superconductivity of (R0.4Pr0.6)0.5Ca0.5Ba2Cu3O7-δ (R = La, Pr, Nd, Sm, Eu, Gd and Y) prepared under high pressure

被引:2
|
作者
Xiong, H [1 ]
Che, GC
Yao, YS
Ni, YM
Liu, ZX
Jia, SL
Dong, C
机构
[1] Chinese Acad Sci, Natl Lab Supercond, Inst Phys, Beijing 100080, Peoples R China
[2] Chinese Acad Sci, Ctr Condensed Matter Phys, Beijing 100080, Peoples R China
关键词
D O I
10.1088/0256-307X/18/5/320
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
The nearly single phase (R0.4Pr0.6)(0.5)Ca0.5Ba2Cu3O7-delta compounds (R = La, Pr, Nd, Sm, Eu, Gd and Y) with T-c about 100K were prepared under high pressure and high temperature using the cubic-anvil apparatus. The T-c is much higher than that of the traditional R-123 superconductors without doping Ca on the rare-earth site. For various rare earths with different ionic radii, the (R0.4Pr0.6)(0.5)Ca0.5Ba2Cu3O7-delta compounds have almost the same critical temperature. This is different from the result of the ion-size effect of rare-earth ions in R1-xPrxBa2Cu3O7-delta compounds. Our results show that Pr has the same properties as other rare earths in the 123-phase compounds due to the doping of Ca.
引用
收藏
页码:684 / 686
页数:3
相关论文
共 50 条
  • [21] Observation of Berezinski-Kosterlitz-Thouless transition in Pr0.6Y0.4Ba2Cu3O7-x/Y1Ba2Cu3O7-x/Pr0.6Y0.4Ba2Cu3O7-x trilayers
    Gasparov, VA
    Batov, IE
    Li, Q
    Kwon, C
    CZECHOSLOVAK JOURNAL OF PHYSICS, 1996, 46 : 1401 - 1402
  • [22] Crystal structure and magnetic properties of R3Co0.5GeS7 (R = Y, La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho, Er and Tm) and R3Ni0.5GeS7 (R = Y, Ce, Sm, Gd, Tb, Dy, Ho, Er and Tm)
    Daszkiewicz, M.
    Pashynska, Yu. O.
    Marchuk, O. V.
    Gulay, L. D.
    Kaczorowski, D.
    JOURNAL OF ALLOYS AND COMPOUNDS, 2015, 647 : 445 - 455
  • [23] Raman spectroscopic study of the La(0.5)R(0.5)Ba(2)Cu(3)O(y) (R=Y, rare earth) superconductors
    Palles, D
    Poulakis, N
    Liarokapis, E
    Gantis, A
    Calamiotou, M
    Koufoudakis, A
    SUPERLATTICES AND MICROSTRUCTURES, 1997, 21 (03) : 329 - 334
  • [24] SUPPRESSION OF SUPERCONDUCTIVITY IN GD1-XPRXBA2CU3O7-Y AND R0.8PR0.2BA2CU3O7-Y SYSTEMS
    YANG, HD
    CHEN, PF
    HSU, CR
    LEE, CW
    LI, CL
    PENG, CC
    PHYSICAL REVIEW B, 1991, 43 (13): : 10568 - 10573
  • [25] Transport properties of the underdoped Y0.5Pr0.5Ba2Cu3O7-δ films in high magnetic fields
    Hao, Z
    Zhao, BR
    Zhu, BY
    Zhao, ZX
    Vanacken, J
    Moshchalkov, VV
    EUROPHYSICS LETTERS, 2002, 58 (01): : 105 - 111
  • [26] The effects of strain, current, and magnetic field on superconductivity in Pr0.5Ca0.5MnO3/YBa2Cu3O7/Pr0.5Ca0.5MnO3 trilayer
    Baisnab, Dipak Kumar
    Janawadkar, M. P.
    Sharma, Shilpam
    Sarguna, R. M.
    Vaidhyanathan, L. S.
    Bharathi, A.
    JOURNAL OF APPLIED PHYSICS, 2013, 113 (11)
  • [27] X-ray rietveld analysis of Y0.4Pr0.6BaSrCu3O7-delta and Y0.4Pr0.6Ba2Cu3O7-delta
    Song, HQ
    Cao, GH
    Yu, YB
    Lu, GL
    Jiao, ZK
    Zhang, QR
    PHYSICA C, 1997, 282 : 759 - 760
  • [28] Interplay between Cu and Fe valences in BaR(Cu0.5Fe0.5)2O5+δ double perovskites with R = Lu, Yb, Y, Eu, Sm, Nd, and Pr
    Lindén, J
    Kochi, M
    Lehmus, K
    Pietari, T
    Karppinen, A
    Yamauchi, H
    JOURNAL OF SOLID STATE CHEMISTRY, 2002, 166 (01) : 118 - 127
  • [29] Structural variation and recovery of superconductivity by Ca substitution in Y0.4Pr0.6Ba2-xCaxCu3O7-delta
    Cao, GH
    Qian, YT
    Wu, HK
    Chen, ZY
    Zhang, YH
    JOURNAL OF SUPERCONDUCTIVITY, 1996, 9 (01): : 89 - 91
  • [30] Crystal structures of the R3Mg0.5GeS7 (R = Y, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho and Er) compounds
    Huch, M.R.
    Gulay, L.D.
    Olekseyuk, I.D.
    Journal of Alloys and Compounds, 2006, 424 (1-2): : 114 - 118