• Observation of ESR in the Bi high-Tc superconductors
    D. Shaltiel, H. Bill, M. Descroux, H. Hagemann, A. Junod, M. Peter, Y. Ravi Sekhar, G. Triscone, E. Walker, Y.F. Yan and Z.X. Zhao
    Physica C: Superconductivity, 157 (2) (1989), p240-246
    DOI:10.1016/0921-4534(89)90008-7 | unige:3067 | Abstract | Article PDF
Electron spin resonance of a high-Tc Bi superconductor sample is reported. The d.c. susceptibility, d.c. resistivity and a.c. susceptibility show two superconducting transitions at 105 K and 75 K. The ESR spectra show a main resonance line whose temperature dependence is studied in detail. The g value shows a maximum of 2.24 at 230 K and decreases to 2.12 at 100 K. The line width also shows a maximum of 520 G at the same temperature and drops to 200 G at 100 K. An unusual behaviour is observed in the decrease of the integrated intensity from a maximum at 230 K to below noise at level 100 K. It is possible that the origin of this signal is due to impurity phases. However, the unusual behaviour of its intensity (disappearance of the signal below Tc) may indicate that it arises from pair formation much above Tc.
  • Single crystal ESR studies on tetragonal YBa2Cu3O6+x
    D. Shaltiel, H. Bill, P. Fischer, M. François, H. Hagemann, M. Peter, Y. Ravi Sekhar, W. Sadowski, H.J. Scheel, G. Triscone, E. Walker and K. Yvon
    Physica C: Superconductivity, 158 (3) (1989), p424-432
    DOI:10.1016/0921-4534(89)90239-6 | unige:3068 | Abstract | Article PDF
We have characterized as-grown and thermally treated YBaCuO single crystals by ESR, Raman spectroscopy, magnetic susceptibility, X-ray and neutron diffraction measurements. The as-grown crystals are tetragonal and are superconducting with an onset temperature of 30 K. They show an ESR signal which behaves as a localized Cu2+ ion with tetragonal symmetry and presumably originates from copper chain atoms that are octahedrally coordinated by six oxygen neighbors. The temperature dependence of the ESR between 150 and 270 K shows paramagnetic behavior and also dynamical features. Below 90 K, the ESR signal disappears reversibly. A likely explanation is that the onset of local superconductivity frustrates the spins responsible for the ESR signal.

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