TY - JOUR
T1 - Flux pinning landscape up to 25 T in SmBa2Cu3Oy films with BaHfO3 nanorods fabricated by low-temperature growth technique
AU - Tsuchiya, Yuji
AU - Miura, Shun
AU - Awaji, Satoshi
AU - Ichino, Yusuke
AU - Matsumoto, Kaname
AU - Izumi, Teruo
AU - Watanabe, Kazuo
AU - Yoshida, Yutaka
N1 - Funding Information:
This research was partially supported by Japan Society for the Promotion of Science (JSPS): Grant-in-Aid for Scientific Research (23226014, 25246032, 26889005, 15H04252, 15K14301, 15H03586, 16J02416, 16K20898), and Japan Science and Technology Agency (JST): Advanced Low Carbon Technology Research and Development Program (ALCA), NU-AIST alliance project. TEM images were taken by Mr S Itoh at IMR, Tohoku Univ.
Publisher Copyright:
© 2017 IOP Publishing Ltd.
PY - 2017/9/4
Y1 - 2017/9/4
N2 - REBa2Cu3Oy superconducting tapes are appropriate for high field magnet applications at low temperatures (i.e. below liquid nitrogen temperature). To clarify the morphology and the volume of the effective pinning center at low temperatures, we used a low-temperature growth technique to fabricate SmBa2Cu3Oy (SmBCO) films with various amounts of BaHfO3 (BHO) nanorods onto MgO-buffered metal substrates produced by ion-beam-assisted deposition; we investigated their flux pinning properties using a 25 T cryogen-free superconducting magnet that was recently developed at Tohoku University. According to the microstructural analysis using transmission electron microscopy, the BHO nanorods have a content-dependent morphology and are aligned for the higher content. The inclined and discontinuous BHO nanorods were observed in SmBCO films with BHO contents up to 3.8 vol%; they show an excellent flux pinning force density (1.5 TN m-3 at 21 T and 4.2 K) even when the magnetic field is perpendicular to the films. Based on the effective mass model for the flux pinning, the random pinning centers are dominant at low temperatures. The correlated flux pinning is stronger for aligned nanorods; however, the random pinning center becomes weaker in the 4.5 vol% BHO-doped films. Therefore, the optimal BHO doping level is approximately 3.8 vol% in terms of the amplitude of the critical current density and the anisotropy from 4.2 K to 20 K because this provides the best mixture of correlated and random flux pinning centers.
AB - REBa2Cu3Oy superconducting tapes are appropriate for high field magnet applications at low temperatures (i.e. below liquid nitrogen temperature). To clarify the morphology and the volume of the effective pinning center at low temperatures, we used a low-temperature growth technique to fabricate SmBa2Cu3Oy (SmBCO) films with various amounts of BaHfO3 (BHO) nanorods onto MgO-buffered metal substrates produced by ion-beam-assisted deposition; we investigated their flux pinning properties using a 25 T cryogen-free superconducting magnet that was recently developed at Tohoku University. According to the microstructural analysis using transmission electron microscopy, the BHO nanorods have a content-dependent morphology and are aligned for the higher content. The inclined and discontinuous BHO nanorods were observed in SmBCO films with BHO contents up to 3.8 vol%; they show an excellent flux pinning force density (1.5 TN m-3 at 21 T and 4.2 K) even when the magnetic field is perpendicular to the films. Based on the effective mass model for the flux pinning, the random pinning centers are dominant at low temperatures. The correlated flux pinning is stronger for aligned nanorods; however, the random pinning center becomes weaker in the 4.5 vol% BHO-doped films. Therefore, the optimal BHO doping level is approximately 3.8 vol% in terms of the amplitude of the critical current density and the anisotropy from 4.2 K to 20 K because this provides the best mixture of correlated and random flux pinning centers.
KW - coated conductors
KW - critical current density
KW - flux pinning
KW - high-temperature superconductor
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U2 - 10.1088/1361-6668/aa7ef0
DO - 10.1088/1361-6668/aa7ef0
M3 - Article
AN - SCOPUS:85032797791
SN - 0953-2048
VL - 30
JO - Superconductor Science and Technology
JF - Superconductor Science and Technology
IS - 10
M1 - 104004
ER -