TY - JOUR
T1 - Critical current densities and irreversibility fields of new high-T-c Ba2CaCu2O4(O,F)(2) superconductor
AU - Shirage, PM
AU - Shivagan, DD
AU - Crisan, Ioan
AU - Tanaka, Y
AU - Kodama, Y
AU - Kito, H
AU - Iyo, A
PY - 2008/1/1
Y1 - 2008/1/1
N2 - Ba2CaCu2O4(O2-yFy) (F-0212), a new high-T-c superconductor (HTSC) including fluorine at an apical site, is an attractive material for application because it shows a highest T-c of 108 K and has thin spacing between conduction layers that is favorable for high critical current density (J(c)) and irreversibility field (B-irr). The polycrystalline samples of F-0212 were synthesized under high pressure. A doping state was controlled from under doping (T-c = 82 K) to slightly-over doping (T-c = 106 K) via optimally-doping (T-c = 108 K). From the DC magnetization hysteresis loops, we determined the intragrain J(c) and B-irr using Bean's critical state model. The J(c) and B-irr properties of F-0212 were found to improve rapidly as the doping state changes from under doping to slightly-over doping to via optimally doping state. The irreversibility lines for the optimally- and slightly-over doped F-0212 are higher than optimally-doped Bi-2212. However, they are much lower than that of Cu-1212 (Y-123) though the spacing of F-0212 is thinner than that of Cu-1212. This indicates that property of the spacing is important to enhance B-irr as well as its thickness. An anisotropy factor for under doped F-0212 was estimated to 118 from a 3D-2D crossover field of about 0.28 T. (C) 2008 Elsevier B.V. All rights reserved.
AB - Ba2CaCu2O4(O2-yFy) (F-0212), a new high-T-c superconductor (HTSC) including fluorine at an apical site, is an attractive material for application because it shows a highest T-c of 108 K and has thin spacing between conduction layers that is favorable for high critical current density (J(c)) and irreversibility field (B-irr). The polycrystalline samples of F-0212 were synthesized under high pressure. A doping state was controlled from under doping (T-c = 82 K) to slightly-over doping (T-c = 106 K) via optimally-doping (T-c = 108 K). From the DC magnetization hysteresis loops, we determined the intragrain J(c) and B-irr using Bean's critical state model. The J(c) and B-irr properties of F-0212 were found to improve rapidly as the doping state changes from under doping to slightly-over doping to via optimally doping state. The irreversibility lines for the optimally- and slightly-over doped F-0212 are higher than optimally-doped Bi-2212. However, they are much lower than that of Cu-1212 (Y-123) though the spacing of F-0212 is thinner than that of Cu-1212. This indicates that property of the spacing is important to enhance B-irr as well as its thickness. An anisotropy factor for under doped F-0212 was estimated to 118 from a 3D-2D crossover field of about 0.28 T. (C) 2008 Elsevier B.V. All rights reserved.
KW - critical current density
KW - irreversibility field
KW - 3D-2D crossover
KW - anisotropy
KW - Ba2CaCu2O4(O,F)(2) superconductor
U2 - 10.1016/j.physc.2007.11.044
DO - 10.1016/j.physc.2007.11.044
M3 - Article
SN - 0921-4534
VL - 468
SP - 773
EP - 776
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - 7-10
ER -