TY - JOUR
T1 - New Fe-based superconductors
T2 - Properties relevant for applications
AU - Putti, M.
AU - Pallecchi, I.
AU - Bellingeri, E.
AU - Cimberle, M. R.
AU - Tropeano, M.
AU - Ferdeghini, C.
AU - Palenzona, A.
AU - Tarantini, C.
AU - Yamamoto, A.
AU - Jiang, J.
AU - Jaroszynski, J.
AU - Kametani, F.
AU - Abraimov, D.
AU - Polyanskii, A.
AU - Weiss, J. D.
AU - Hellstrom, E. E.
AU - Gurevich, A.
AU - Larbalestier, D. C.
AU - Jin, R.
AU - Sales, B. C.
AU - Sefat, A. S.
AU - McGuire, M. A.
AU - Mandrus, D.
AU - Cheng, P.
AU - Jia, Y.
AU - Wen, H. H.
AU - Lee, S.
AU - Eom, C. B.
PY - 2010
Y1 - 2010
N2 - Less than two years after the discovery of high temperature superconductivity in oxypnictide LaFeAs(O, F) several families of superconductors based on Fe layers (1111, 122, 11, 111) are available. They share several characteristics with cuprate superconductors that compromise easy applications, such as the layered structure, the small coherence length and unconventional pairing. On the other hand, the Fe-based superconductors have metallic parent compounds and their electronic anisotropy is generally smaller and does not strongly depend on the level of doping, and the supposed order parameter symmetry is s-wave, thus in principle not so detrimental to current transmission across grain boundaries. From the application point of view, the main efforts are still devoted to investigate the superconducting properties, to distinguish intrinsic from extrinsic behaviors and to compare the different families in order to identify which one is the fittest for the quest for better and more practical superconductors. The 1111 family shows the highest T c, huge but also the most anisotropic upper critical field and in-field, fan-shaped resistive transitions reminiscent of those of cuprates. On the other hand, the 122 family is much less anisotropic with sharper resistive transitions as in low temperature superconductors, but with about half the Tc of the 1111 compounds. An overview of the main superconducting properties relevant to applications will be presented. Upper critical field, electronic anisotropy parameter, and intragranular and intergranular critical current density will be discussed and compared, where possible, across the Fe-based superconductor families.
AB - Less than two years after the discovery of high temperature superconductivity in oxypnictide LaFeAs(O, F) several families of superconductors based on Fe layers (1111, 122, 11, 111) are available. They share several characteristics with cuprate superconductors that compromise easy applications, such as the layered structure, the small coherence length and unconventional pairing. On the other hand, the Fe-based superconductors have metallic parent compounds and their electronic anisotropy is generally smaller and does not strongly depend on the level of doping, and the supposed order parameter symmetry is s-wave, thus in principle not so detrimental to current transmission across grain boundaries. From the application point of view, the main efforts are still devoted to investigate the superconducting properties, to distinguish intrinsic from extrinsic behaviors and to compare the different families in order to identify which one is the fittest for the quest for better and more practical superconductors. The 1111 family shows the highest T c, huge but also the most anisotropic upper critical field and in-field, fan-shaped resistive transitions reminiscent of those of cuprates. On the other hand, the 122 family is much less anisotropic with sharper resistive transitions as in low temperature superconductors, but with about half the Tc of the 1111 compounds. An overview of the main superconducting properties relevant to applications will be presented. Upper critical field, electronic anisotropy parameter, and intragranular and intergranular critical current density will be discussed and compared, where possible, across the Fe-based superconductor families.
UR - http://www.scopus.com/inward/record.url?scp=77649139801&partnerID=8YFLogxK
U2 - 10.1088/0953-2048/23/3/034003
DO - 10.1088/0953-2048/23/3/034003
M3 - Article
AN - SCOPUS:77649139801
SN - 0953-2048
VL - 23
JO - Superconductor Science and Technology
JF - Superconductor Science and Technology
IS - 3
M1 - 034003
ER -