Abstract
We examine the effects of disorder on striped phases in high-temperature superconductors and related materials. In the presence of quenched disorder pinning, by the atomic lattice—which might give rise to commensuration effects—is irrelevant for two-dimensional stripe arrays on large length scales. As a consequence, the stripes have divergent displacement fluctuations and topological defects are present at all temperatures. Therefore, the positional order of the stripe array is short ranged with a finite correlation length even at zero temperature. Thus lock-in phenomena can exist only as crossovers but not as transitions. In addition, this implies the glassy nature of stripes observed in recent experiments.
- Received 17 January 2001
DOI:https://doi.org/10.1103/PhysRevB.64.054517
©2001 American Physical Society