Doping dependence of the upper critical field, superconducting current density and thermally activated flux flow activation energy in polycrystalline CeFeAsO1-xFx superconductors

被引:8
作者
Chong, S. V. [1 ,2 ]
Williams, G. V. M. [2 ,3 ]
Sambale, S. [1 ,3 ]
Kadowaki, K. [4 ]
机构
[1] Victoria Univ Wellington, Robinson Res Inst, Lower Hutt 5046, New Zealand
[2] Victoria Univ Wellington, MacDiarmid Inst Adv Mat & Nanotechnol, Wellington 6140, New Zealand
[3] Victoria Univ Wellington, Sch Chem & Phys Sci, Wellington 6140, New Zealand
[4] Univ Tsukuba, Fac Pure & Appl Sci, Div Mat Sci, Tsukuba, Ibaraki 3058573, Japan
来源
PHYSICA C-SUPERCONDUCTIVITY AND ITS APPLICATIONS | 2014年 / 507卷
关键词
Iron-based superconductors; Quaternary compound; Flux flow activation energy; Critical current density; Maki parameter; PHASE-DIAGRAM; TEMPERATURE; MAGNETIZATION; PSEUDOGAP;
D O I
10.1016/j.physc.2014.09.015
中图分类号
O59 [应用物理学];
学科分类号
摘要
We report the results from resistivity and magnetic measurements on polycrystalline Ce oxypnictide (CeFeAsO1-xFx) samples where x spans from 0.13 to 0.25. We find that the orbital limiting field is as high as 150 T and it systematically decreases with increasing doping. The Maki parameter is greater than one across the phase diagram and the large Maki parameter suggests that orbital and Pauli limiting effects contribute to the upper critical field. The broadening of the superconducting transition in the resistivity data was interpreted using the thermally activated flux flow (TAFF) model where we find that the TAFF activation energy, U-0(B), is proportional to B (gamma) from 1 T to high fields, and gamma does not significantly change with doping. However, U-0 and the superconducting critical current, J(c), are peaked in the mid-doping region (x = 0.15-0.20), and not in the low (x < 0.15) or high doping (x > 0.20) regions. Furthermore, U-0 is correlated with Jc and follows the two fluid model for granular samples. (C) 2014 Elsevier B.V. All rights reserved.
引用
收藏
页码:35 / 40
页数:6
相关论文
共 55 条
[1]   An overview on iron based superconductors [J].
Aswathy, P. M. ;
Anooja, J. B. ;
Sarun, P. M. ;
Syamaprasad, U. .
SUPERCONDUCTOR SCIENCE & TECHNOLOGY, 2010, 23 (07)
[2]   MAGNETIZATION OF HIGH-FIELD SUPERCONDUCTORS [J].
BEAN, CP .
REVIEWS OF MODERN PHYSICS, 1964, 36 (1P1) :31-+
[3]   VORTICES IN HIGH-TEMPERATURE SUPERCONDUCTORS [J].
BLATTER, G ;
FEIGELMAN, MV ;
GESHKENBEIN, VB ;
LARKIN, AI ;
VINOKUR, VM .
REVIEWS OF MODERN PHYSICS, 1994, 66 (04) :1125-1388
[4]   THE FLUX-LINE-LATTICE IN SUPERCONDUCTORS [J].
BRANDT, EH .
REPORTS ON PROGRESS IN PHYSICS, 1995, 58 (11) :1465-1594
[5]   GIANT SUPPRESSION OF FLUX-FLOW RESISTIVITY IN HEAVY-ION IRRADIATED TL2BA2CA2CU3O10 FILMS - INFLUENCE OF LINEAR DEFECTS ON VORTEX TRANSPORT [J].
BUDHANI, RC ;
SUENAGA, M ;
LIOU, SH .
PHYSICAL REVIEW LETTERS, 1992, 69 (26) :3816-3819
[6]   LIMITS TO THE CRITICAL-CURRENT IN HIGH-T(C) SUPERCONDUCTING TAPES [J].
BULAEVSKII, LN ;
DAEMEN, LL ;
MALEY, MP ;
COULTER, JY .
PHYSICAL REVIEW B, 1993, 48 (18) :13798-13816
[7]   Superconductivity at 41 K and its competition with spin-density-wave instability in layered CeO1-xFxFeAs [J].
Chen, G. F. ;
Li, Z. ;
Wu, D. ;
Li, G. ;
Hu, W. Z. ;
Dong, J. ;
Zheng, P. ;
Luo, J. L. ;
Wang, N. L. .
PHYSICAL REVIEW LETTERS, 2008, 100 (24)
[8]   Various regimes of flux motion in Bi2Sr2CaCu2O8+δ single crystals [J].
Chen, WM ;
Franck, JP ;
Jung, J .
PHYSICA C, 2000, 341 :1195-1196
[9]  
Chong SV, 2008, J PHYS SOC JPN, V77, P27
[10]   UPPER LIMIT FOR CRITICAL FIELD IN HARD SUPERCONDUCTORS [J].
CLOGSTON, AM .
PHYSICAL REVIEW LETTERS, 1962, 9 (06) :266-&