dc.contributor | Universidade Estadual Paulista (UNESP) | |
dc.contributor | Universidade Federal do Rio de Janeiro (UFRJ) | |
dc.date.accessioned | 2022-04-28T20:07:44Z | |
dc.date.accessioned | 2022-12-20T01:53:28Z | |
dc.date.available | 2022-04-28T20:07:44Z | |
dc.date.available | 2022-12-20T01:53:28Z | |
dc.date.created | 2022-04-28T20:07:44Z | |
dc.date.issued | 2006-05-31 | |
dc.identifier | Physical Review B - Condensed Matter and Materials Physics, v. 73, n. 19, 2006. | |
dc.identifier | 1098-0121 | |
dc.identifier | 1550-235X | |
dc.identifier | http://hdl.handle.net/11449/224759 | |
dc.identifier | 10.1103/PhysRevB.73.193407 | |
dc.identifier | 2-s2.0-33646866606 | |
dc.identifier.uri | https://repositorioslatinoamericanos.uchile.cl/handle/2250/5404888 | |
dc.description.abstract | We discuss the interplay between electronic correlations and an underlying superlattice structure in determining the period of charge density waves (CDW's), by considering a one-dimensional Hubbard model with a repeated (nonrandom) pattern of repulsive (U>0) and free (U=0) sites. Density matrix renormalization group diagonalization of finite systems (up to 120 sites) is used to calculate the charge-density correlation function and structure factor in the ground state. The modulation period can still be predicted through effective Fermi wave vectors kF* and densities, and we have found that it is much more sensitive to electron (or hole) doping, both because of the narrow range of densities needed to go from q* =0 to π, but also due to sharp 2 kF* -4 kF* transitions; these features render CDW's more versatile for actual applications in heterostructures than in homogeneous systems. © 2006 The American Physical Society. | |
dc.language | eng | |
dc.relation | Physical Review B - Condensed Matter and Materials Physics | |
dc.source | Scopus | |
dc.title | Modulation of charge-density waves by superlattice structures | |
dc.type | Artículos de revistas | |