Duong Thi Thanh Nhan, Tran Hai Duc

Main Article Content

Abstract

Abstract: Effect of BaSnO3 (BSO) nanoparticle inclusion on the critical current density of GdBa2Cu3O7-x (GdBCO) thin films was investigated. BSO nanoparticles were prepared on a thin GdBCO seed layer of < 50 nm thick by using pulsed laser deposition (PLD) technique. The GdBCO superconducting layers were deposited on top of the BSO nanoparticles to produce films with the entire thickness of approximately 250 nm[O1] . The number of laser pulses was varied from 20 to 320 in order to obtain BSO nanoparticles with different sizes and densities. Magnetization data measured at 65 K showed that: at a small number of laser pulses, the slight enhancement in critical current density (Jc) up to 1.5 T was obtained. Further increasing the number of laser pulses, Jcs were found to be consistently decreased. The increase in Jc was attributed to the addition of BSO nanoparticles serving as artificial pinning centers (APCs) inside GdBCO films. The decreases in Jc was probably caused by to the crystallinity degradation of the BSO-doped GdBCO films which was confirmed by the larger FHWM values.

Keywords: GdBCO thin film, critical current density, BaSnO3, artificial pinning centers.

 [O1]

References

[1] Y. Xu, M. Izumi, K. Tsuzuki, Y. Zhang, C. Xu, M. Murakami, N. Sakai and I. Hirabayashi, Thickness dependence of critical current density in GdBa2Cu3O7−δ thin films with BaSnO3 addition, Supercond. Sci. Technol, 22, 095009, (2009).
[2] S. Rosenzweig, J. Hänisch, K. Iida, A. Kauffmann, Ch. Mickel, T. Thersleff, J. Freudenberger, R. Hühne, B. Holzapfel and L. Schultz, Thickness dependence of critical current density in GdBa2Cu3O7−δ thin films with BaSnO3 addition, Supercond. Sci. Technol, 23, 105017, (2010).
[3] M. Murakami, N. Sakai, T. Higuchi and S.I. Yoo, Melt-processed light rare earth element-Ba-Cu-O Supercond. Sci. Technol, 9, 1015 (1996).
[4] K. Matsumoto and P. Mele, Artificial pinning center technology to enhance vortex pinning in YBCO coated conductors, Supercond. Sci. Technol, 23, 014001 (2010).
[5] D.H. Tran, W.B.K. Putri, C.H. Wie, B. Kang, N.H. Lee, W.N. Kang, J.Y. Lee, and W.K. Seong, Thickness dependence of critical current density in GdBa2Cu3O7−δ thin films with BaSnO3 addition, J. Appl. Phys, 111, 07D714 (2012).
[6] D.H. Tran, W.B.K. Putri, C.H. Wie, B. Kang, N.H. Lee, W.N. Kang, J.Y. Lee and W.K. Seong, Enhanced critical current density in GdBa2Cu3O7-δ thin films with substrate surface decoration using Gd2O3 nanoparticles ", Thin Solid Films 526, 241 (2012).
[7] P. Mele, K. Matsumoto, T. Horide, O. Miura, A. Ichinose, M. Mukaida, Y. Yoshita, and S. Horii, Control of Y2O3 nanoislands deposition parameters in order to induce defects formation and its influence on the critical current density of YBCO films, Physica C, 426-431, 1108 (2005).
[8] P. Mikheenko, A. Sarkar, V.S. Dang, J.L. Tanner, J.S.Abell, and A. Crisan, c-Axis correlated extended defects and critical current in YBa2Cu3Ox films grown on Au and Ag-nano dot decorated substrates, Physica C, 469, 798 (2009).
[9] P. N. Barnes, T. J. Haugan, C. V. Varanasi and T. A. Campbell, Flux pinning behavior of incomplete multilayered lattice structures in YBa2Cu3O7−d, Appl. Phys. Lett, 85, 4088 (2004).