Studies on ac losses in Bi2SR2CaCu2O8 single crystals

• Published in: Physica. C, Superconductivity Vol. 460-462; no. 2; pp. 719 - 721
• Main Authors: CHOCKALINGAM, S. P, SARANGI, S, BHAT, S. V, OKA, K, NISHIHARA, Y
• Format: Conference Proceeding Journal Article
• Language: English
• Published: Amsterdam Elsevier Science 01.09.2007
• Subjects: Condensed matter: electronic structure, electrical, magnetic, and optical properties; Critical currents; Cuprates superconductors (high tc and insulating parent compounds); Exact sciences and technology; Physics; Properties of type I and type II superconductors; Superconductivity; Vortex lattices ,flux pinning, flux creep; Critical current density; Bi2Sr2CaCu2O8; Superconductivity; Magnetic field effects; Bismuth oxides; Radiofrequency; Calcium oxides; Strontium oxides; Monocrystals; Josephson effect; Vortices; High-Tc superconductors; Vortex motion; Josephson junctions; AC losses; Copper oxides
• ISSN: 0921-4534; 1873-2143
• DOI: 10.1016/j.physc.2007.03.150

Using a novel technique of measuring absolute ac losses at radio frequencies, the temperature, magnetic field and angle dependence of rf losses in superconducting single crystals of Bi2Sr2CaCu2O8 is studied. An unexpected, larger than normal state ac loss is observed below Tc. We provide an explanation for this observation in terms of the energy required to decouple the intrinsic Josephson junctions in the crystals. The studies are carried out both at zero magnetic field and at different values of magnetic fields applied at different angles theta between the field and the c-axis of the crystal. We observe two maxima in ac loss as a function of temperature. The amplitude, width and the position of the first maximum (peak A) change with the magnitude and orientation of the applied magnetic field. These results are discussed in terms of the critical current density of the Josephson junctions, which decreases with the increasing field and changes with the orientation. The second maximum (peak B) appears just below Tc only in the presence of the magnetic field and has been attributed to the vortex motion. The amplitude of this peak as well changes with the magnetic field and with the angle of orientation. The analysis shows that the loss is due to pancake vortices.