APS March Meeting 2015
Volume 60, Number 1
Monday–Friday, March 2–6, 2015;
San Antonio, Texas
Session J11: Focus Session: Engineering Vortex Matter in Superconductors I
2:30 PM–5:30 PM,
Tuesday, March 3, 2015
Room: 007B
Sponsoring
Unit:
DMP
Chair: Ulrich Welp, Argonne National Laboratory
Abstract ID: BAPS.2015.MAR.J11.7
Abstract: J11.00007 : Development of strong vortex pinning and very high $J_{c}$ in iron based superconductors
3:42 PM–4:18 PM
Preview Abstract
Abstract
Author:
Chiara Tarantini
(National High Magnetic Field Laboratory - Florida State University)
Ba(Fe$_{\mathrm{1-x}}$Co$_{\mathrm{x}})_{2}$As$_{2}$
(Ba122) is the most tunable of the Fe-based superconductors (FBS) in terms
of its acceptance of high densities of secondary phases capable of acting as
effective pinning centers without depressing the properties of the
superconducting matrix. It has been demonstrated that self-assembled
nanorods made of Ba-Fe-O generate a strong correlated pinning along the
c-axis, enhancing the critical current density, $J_{c}$, in this direction
and reducing the $J_{c}$ anisotropy [1, 2]. However, when 20{\%} of secondary
phases are introduced, the reduction of the cross-section becomes
significant, decreasing the low field performance. In order to overcome this
issue, artificially introduced pinning centers can be added by multilayer
deposition producing an almost isotropic increase of $J_{c}$ [2]. Moreover,
FBS are very sensitive to strain, allowing an important enhancement in the
critical temperature, $T_{c}$, of the material. It will be shown that strain
induced by the substrate can further improve $J_{c}$ of both single and
multilayer films by more than expected because of the $T_{c}$ increase. The
multilayer deposition of Ba122 on CaF$_{2}$ increases the pinning
force density, $F_{p}$, by more than 60{\%} compared to a single layer film,
reaching a maximum of 84 GN/m$^{3}$ at 22.5T and 4.2 K, the highest
value ever reported in any 122 phase. This work shows that the in-field
performance of Ba122 widely exceeds that of Nb$_{3}$Sn above 10T,
attracting attention for possible applications.
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[1] C. Tarantini, S. Lee, Y. Zhang, J. Jiang, C.W. Bark, J.D. Weiss, A. Polyanskii, C.T. Nelson, H.W. Jang, C.M. Folkman, S.H. Baek, X.Q. Pan, A. Gurevich, E.E. Hellstrom, C.B.
Eom, D.C. Larbalestier, Appl.Phys.Lett. 96, 142510 (2010)
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[2] C. Tarantini, S. Lee, F. Kametani, J. Jiang, J.D. Weiss, J. Jaroszynski, C.M. Folkman, E.E. Hellstrom, C.B. Eom, D.C. Larbalestier, Phys.Rev.B 86, 214504 (2012)
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[3] C. Tarantini, F. Kametani, S. Lee, J. Jiang, J.D. Weiss, J. Jaroszynski, E.E. Hellstrom, C.B. Eom, D.C. Larbalestier, Scientific Reports (2014)
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2015.MAR.J11.7