Fragmentation of bands and the Fermi surfaces in stripe phases
arXiv:cond-mat/0407767 · doi:10.1209/epl/i2004-10352-9
Abstract
The mean-field study of the stripe phases of t-t'-U Hubbard model confirms formation of the "impurity" subbands of states localized on domain walls. For bond-aligned stripes it is shown that segments of the Fermi surfaces (FS) in antinodal and nodal directions correspond to the "impurity" band or to that delocalized over a whole antiferromagnet domain. This might explain the dichotomy between corresponding quasiparticles in La_{2-x}Sr_xCuO_4. The Fermi surface changes its topology at some doping depending on stripe width. Additional ordering at the domain walls should be supposed to accord the observed 1/8 anomaly and the stripe spacing. It is confirmed also that the diagonal stripes can provide the dielectric state at nonzero doping.
7 pages, 4 figures
References in corpus (8)
- Angle-resolved photoemission spectroscopy of the cuprate superconductors
- How to detect fluctuating order in the high-temperature superconductors
- Stripe order, depinning, and fluctuations in LaBaCuO and LaBaSrCuO
- The Dichotomy between Nodal and Antinodal Quasiparticles in Underdoped (LaSr)CuO Superconductors
- Metallic mean-field stripes, incommensurability and chemical potential in cuprates
- Dynamics of metallic stripes in cuprates
- Stability of metallic stripes in the extended one-band Hubbard model
- Band structure of Charge Ordered Doped Antiferromagnets