Abstract
We study disorder-induced magnetism within the Gutzwiller approximation applied to the t-J model relevant for cuprate superconductors. In particular, we show how disorder generates magnetic phases by inducing local droplets of antiferromagnetic order which eventually merge and form a quasi-long-range ordered state in the underdoped regime. We identify two distinct disorder-induced magnetic phases of this type depending on the strength of the scatterers. For weak potential scatterers used to model dopant disorder, charge reorganization may push local regions in between the impurities across the magnetic phase boundary, whereas for strong scatterers used to model substitutional ions, a local static magnetic moment is formed around each impurity. We calculate the density of states and find a remarkably universal low-energy behavior largely independent of both disorder and magnetization. However, the magnetic regions are characterized by larger (reduced) superconducting gap (coherence peaks) and a subgap kink in the density of states.
Originalsprog | Engelsk |
---|---|
Tidsskrift | Physical Review B. Condensed Matter and Materials Physics |
Vol/bind | 84 |
Udgave nummer | 18 |
Sider (fra-til) | 184511 |
ISSN | 2469-9950 |
DOI | |
Status | Udgivet - 14 nov. 2011 |