Presentation Information

[WB4-04]Co-doping with BaSnO3 and BaHfO3 by Ultra-high Rate PLD Enabling Formation of High-density Nanocolumns in EuBa2Cu3O7-δ Films

*Yue Wu1, Mengrui Zhao1, Chunsheng Chen2, Yuji Tsuchiya3, Tatsunori Okada4, Junyi Luo3, Satoshi Awaji3, Yue Zhao1,2 (1. Shanghai Jiao Tong University (China), 2. SuperMag Tehcnology (Shanghai) Co., Ltd. (China), 3. Institute for Materials Research, Tohoku University (Japan), 4. Department of Materials Science and Engineering, Kyushu Institute of Technology (Japan))
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Keywords:

High-temperature superconductor,Pulse laser deposition,Defects engineering,Diffusion,Nanocolumns

Introduction of artificial pinning centers through defects engineering is an effective strategy to mitigate the reduction of in-field current carrying capacity of REBCO tapes. However, it is challenging for formation of high-density columnar secondary phase while maintaining the high crystallinity of REBCO at high-speed deposition during the pulsed laser deposition (PLD) process, which restricts mass production of high-performance tapes for high-field magnet applications. In this work, a BaHfO3+BaSnO3 co-dopant strategy was utilized to modulate the microstructure of doped EuBa2Cu3O7-δ (EuBCO) films via reel-to-reel multi-plume and multi-turn PLD with ultra-high rate (exceeding 100 nm/s). These nanocolumnar structures, composed of BaSnxHf1-xO3 (BSHO) at the atomic scale, were aligned along the thickness direction throughout the EuBCO layer. The high-density nanocolumns, ∼ 5 nm diameter, exhibited an areal density of about 2200 pieces/μm2 . This unique microstructure significantly enhanced the in-field Jc of co-doped film. At 50 K and 3 T, the Jc reaches ∼4.0 MA/cm2 at perpendicular field, exceeding that at parallel field. Notably, even under a higher field (50 K and 8 T), the Jc(θ) curve of the co-doped film exhibits a pronounced correlated pinning peak in the perpendicular field. The large in-plane lattice mismatch between the BSHO and EuBCO leads to the formation of semi-coherent interfaces, which introduce numerous nanoscale defects acting as random pinning centers under high fields. High-field superconductivity measurement results indicate that the pinning force displays non-saturation phenomenon at 4.2 K up to 24 T, achieving a high value of ∼990 GN/m3 .