Back to Search Start Over

Small anisotropy, weak thermal fluctuations, and high field superconductivity in Co-doped iron pnictide Ba(Fe1-xCox)2As2.

Authors :
Yamamoto, A.
Jaroszynski, J.
Tarantini, C.
Balicas, L.
Jiang, J.
Gurevich, A.
Larbalestier, D. C.
Jin, R.
Sefat, A. S.
McGuire, M. A.
Sales, B. C.
Christen, D. K.
Mandrus, D.
Source :
Applied Physics Letters; 2/9/2009, Vol. 94 Issue 6, pN.PAG, 3p, 5 Graphs
Publication Year :
2009

Abstract

We performed high-field magnetotransport and magnetization measurements on a single crystal of the 122-phase iron pnictide Ba(Fe<subscript>1-x</subscript>Co<subscript>x</subscript>)<subscript>2</subscript>As<subscript>2</subscript>. Unlike the high-temperature superconductor cuprates and 1111-phase oxypnictides, Ba(Fe<subscript>1-x</subscript>Co<subscript>x</subscript>)<subscript>2</subscript>As<subscript>2</subscript> showed practically no broadening of the resistive transitions under magnetic fields up to 45 T. We report the temperature dependencies of the upper critical field H<subscript>c2</subscript> both parallel and perpendicular to the c-axis, the irreversibility field H<subscript>irr</subscript><superscript>c</superscript>(T), and a rather unusual symmetric volume pinning force curve F<subscript>p</subscript>(H) suggestive of a strong pinning nanostructure. The anisotropy parameter γ=H<subscript>c2</subscript><superscript>ab</superscript>/H<subscript>c2</subscript><superscript>c</superscript> deduced from the slopes of dH<subscript>c2</subscript><superscript>ab</superscript>/dT=4.9 T/K and dH<subscript>c2</subscript><superscript>c</superscript>/dT=2.5 T/K decreases from ∼2 near T<subscript>c</subscript>, to ∼1.5 at lower temperatures, much smaller than γ for 1111pnictides and high-T<subscript>c</subscript> cuprates. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
00036951
Volume :
94
Issue :
6
Database :
Complementary Index
Journal :
Applied Physics Letters
Publication Type :
Academic Journal
Accession number :
36609451
Full Text :
https://doi.org/10.1063/1.3081455