The Y 1-xHo xBa-2Cu-3O y superconductors were fabricated by the powder melting process (PMP) method and the magnetic hysteresis loops of these samples were measured at different temperatures by a SQUID magnetometer (u...The Y 1-xHo xBa-2Cu-3O y superconductors were fabricated by the powder melting process (PMP) method and the magnetic hysteresis loops of these samples were measured at different temperatures by a SQUID magnetometer (up to 7 T). Critical current density was calculated by the Bean critical state model. The results indicate that the fishtail effect is observed in Y 0.6Ho 0.4Ba-2Cu-3O y below 60 K, while no fishtail can be found in Y 0.8Ho 0.2Ba-2Cu-3O y until 30 K. The peak field at which J c reaches its maximum decreases with the increasing magnetic field. In the Y 0.6Ho 0.4Ba-2Cu-3O y sample, the fishtail effect disappears when the temperature is raised to 77 K. In addition, after the Y 0.6Ho 0.4Ba-2Cu-3O y sample was re-sintered at high temperature for a long time, the fishtail can be found in two field directions (H∥C and H⊥C). It is considered that the paramagnetism in the sample may be responsible for the fishtail effect in Ho-added YBCO. Also, the cation disorder created by Ho addition may be another reason for the fishtail.展开更多
文摘The Y 1-xHo xBa-2Cu-3O y superconductors were fabricated by the powder melting process (PMP) method and the magnetic hysteresis loops of these samples were measured at different temperatures by a SQUID magnetometer (up to 7 T). Critical current density was calculated by the Bean critical state model. The results indicate that the fishtail effect is observed in Y 0.6Ho 0.4Ba-2Cu-3O y below 60 K, while no fishtail can be found in Y 0.8Ho 0.2Ba-2Cu-3O y until 30 K. The peak field at which J c reaches its maximum decreases with the increasing magnetic field. In the Y 0.6Ho 0.4Ba-2Cu-3O y sample, the fishtail effect disappears when the temperature is raised to 77 K. In addition, after the Y 0.6Ho 0.4Ba-2Cu-3O y sample was re-sintered at high temperature for a long time, the fishtail can be found in two field directions (H∥C and H⊥C). It is considered that the paramagnetism in the sample may be responsible for the fishtail effect in Ho-added YBCO. Also, the cation disorder created by Ho addition may be another reason for the fishtail.
