Abstract
Synchrotron x-ray diffraction measurements on a high purity single crystal reveal that the absence of long-range ortho-II order in YBC is most likely due to random-field effects. The ortho-II superstructure peaks show three qualitative features consistent with random-field behavior: First, instead of the development of a sharp Bragg peak at the transition °C (for ), the initial diffuse anisotropic Lorentzian (critical scattering) above transforms to a Lorentzian-squared form below . Second, the equilibration time increases dramatically at the onset of ordering. And third, the domain growth is logarithmic in time below .
- Received 3 October 1994
DOI:https://doi.org/10.1103/PhysRevLett.74.1446
©1995 American Physical Society