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Extra resources for Advances in Superconductivity V: Proceedings of the 5th International Symposium on Superconductivity (ISS ’92), November 16–19, 1992, Kobe
5) The error in the previous results is in sample preparation, in which insufficient treatment times and inappropriate treatment temperatures were employed. 2. This transition occurs in many other K 2 NiF 4 structure materials and is typical of those found in many perovskites. It is therefore not likely to be driven by the same forces that give rise to high T c superconductivity. In my opinion, the symmetry transition is happening independently of superconductivity, and the changes in bonding angles that occur at the transition are enough to destroy superconductivity in the tetragonal phase.
For the downward kink in Fig. 6 no straightforward explanation can be found. As shown in Fig. 1 T, where jc in the sample exhibits again a "pure" linear Bi(2223) behavior. It should be stressed here that the changes in slope reported here are not due to sample selfheating or to other experimental errors. Moreover, they were observed on several tapes. 21 Ie [A] • 15 I--~~~~'c--+--+--f 20 40 60 80 100 T[K] Fig. 7. Suppression of the downward kink inje at - SOK by applying H /I surface [S]. The temperature dependence of je for a Bi(2223) tape (Fig.
MIYAJIMA, Y. OTANI, Y. ISHIKAWA, S. YOSHIZAWA .............................................................................. 1277 On Coupling Coefficient of Mutual Inductance with Bi System Core Under External DC Magnetic Field K. HOTTA, K. FUNATO, H. HIROSE ................................................ 1281 Measurements of Magnetic Field Shielding Effects of NbTi-Cu Multilayer Films by a SQUID-Based Magnetometer K. NISHIGAKI, A. FUJISHIRO, M. TAKEDA, S. OGAWA, M. SATO, M. INOUE ......................................................................