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When investigating low-frequency (0.1 Hz) oscillations of miltiphase high-temperature cuprate superconductors (HTSC) Bi1,7Pb0,3Sr2Ca(n-1)CunOy (n=2-30), a wide attenuation peak with a maximal at T=200K detected. This peak was particularly pronounced in field cooling (FC) experiments, i.e. after abrupt cooling of the sample in the external magnetic field at the temperature T less Tc with subsequent slow warming up to room temperature with invariance of applied field. The attenuation peak height depended on the preliminary orientation (before cooling) of the samples in the measured permanent magnetic field H. On the one hand, it is well khow that, after the FC procedure and subsequent slow warming up, at the temperatures close to the critical temperature Tc, the attenuation peak associated with melting of the Abrikosov frozen vortex structure and its disappearance at T more Tc is detected in monophase samples. At the same time, in most multiphase bismuth HTSC samples, synthesized using solar energy and superfast quenching of the melt, the attenuation peak with the maximum at T=200K was observed. Depending on the conditions of synthesis, the attenuation peak could be two-humped and could be located in the temperature range much wider than Tc of the major superconducting phase. We assume that this is due to the existence of frozen magnetic fluxes (after FC) in superconducting dropping regions, which gradually (with increasing temperature) transfer into the normal state and release pinned vortex threads. This fact could be a sause of observed dissipative processes, so as also the evidence of the existence of superconductivity at T more 240K.
Unconventional superconductivity has been suggested to be present at the interface between bismuth and nickel in thin-film bilayers. In this work, we study the structural, magnetic and superconducting properties of sputter deposited Bi/Ni bilayers. A
Using a membrane-driven diamond anvil cell and both ac magnetic susceptibility and electrical resistivity measurements, we have characterized the superconducting phase diagram of elemental barium to pressures as high as 65 GPa. We have determined the
Very recent report [1] on observation of superconductivity in Bi4O4S3 could potentially reignite the search for superconductivity in a broad range of layered sulphides. We report here synthesis of Bi4O4S3 at 5000C by vacuum encapsulation technique an
One of the central questions in the cuprate research is the nature of the normal state which develops into high temperature superconductivity (HTSC). In the normal state of hole-doped cuprates, the existence of charge density wave (CDW) is expected t
The discovery of high temperature superconductivity in the cuprates in 1986 triggered a spectacular outpouring of creative and innovative scientific inquiry. Much has been learned over the ensuing 28 years about the novel forms of quantum matter that