Explanation of delocalization in the continuous random-dimer model
dc.contributor.author | Sánchez, Angel | |
dc.contributor.author | Domínguez-Adame Acosta, Francisco | |
dc.contributor.author | Berman, Gennady P. | |
dc.contributor.author | Izrailev, Felix | |
dc.date.accessioned | 2023-06-20T19:12:38Z | |
dc.date.available | 2023-06-20T19:12:38Z | |
dc.date.issued | 1995-03-01 | |
dc.description | © 1995 The American Physical Society. A.S. was partially supported by MEC (Spain)/Fulbright, by DGICyT (Spain) through project PB92-0248, and by the European Union Human Capital and Mobility Programme through Contract No. ERBCHRXCT930413. F.D.-A. was supported by Universidad Complutense through project PR161/93-4811. G.P.B. gratefully acknowledges partial support from Linkage Grant No. 93-1602 from NATO Special Programme Panel on Nanotechnology. Work at Los Alamos is performed under the auspices of the U.S. Department of Energy. | |
dc.description.abstract | We propose an explanation of the bands of extended states appearing in random one-dimensional models with correlated disorder, focusing on the continuous random-dimer model [A. Sanchez, E. Macia, and F. Dominguez-Adame, Phys. Rev. B 49, 147 (1994)].We show exactly that the transmission coefficient at the resonant energy is independent of the number of host sites between two consecutive dimers. This allows us to understand why there are bands of extended states for every realization of the model as well as the dependence of the bandwidths on the concentration. We carry out a perturbative calculation that sheds more light on the above results. In the conclusion we discuss generalizations of our results to other models and possible applications which arise from insight into this problem. | |
dc.description.department | Depto. de Física de Materiales | |
dc.description.faculty | Fac. de Ciencias Físicas | |
dc.description.refereed | TRUE | |
dc.description.sponsorship | MEC (Spain) | |
dc.description.sponsorship | DGICyT (Spain) | |
dc.description.sponsorship | Universidad Complutense | |
dc.description.sponsorship | NATO | |
dc.description.status | pub | |
dc.eprint.id | https://eprints.ucm.es/id/eprint/28029 | |
dc.identifier.doi | 10.1103/PhysRevB.51.6769 | |
dc.identifier.issn | 0163-1829 | |
dc.identifier.officialurl | http://dx.doi.org/10.1103/PhysRevB.51.6769 | |
dc.identifier.relatedurl | http://journals.aps.org | |
dc.identifier.uri | https://hdl.handle.net/20.500.14352/59394 | |
dc.issue.number | 10 | |
dc.journal.title | Physical Review B | |
dc.language.iso | eng | |
dc.page.final | 6772 | |
dc.page.initial | 6769 | |
dc.publisher | American Physical Society | |
dc.relation.projectID | PB92-0248 | |
dc.relation.projectID | PR161/93-4811 | |
dc.relation.projectID | 93-1602 | |
dc.relation.projectID | ERBCHRXCT930413 | |
dc.rights.accessRights | open access | |
dc.subject.cdu | 538.9 | |
dc.subject.keyword | Localization | |
dc.subject.keyword | Absence | |
dc.subject.ucm | Física de materiales | |
dc.title | Explanation of delocalization in the continuous random-dimer model | |
dc.type | journal article | |
dc.volume.number | 51 | |
dcterms.references | 1. J. C. Flores, J. Phys. Condens. Matter 1, 8471 (1989). 2. D. H. Dunlap, H.-L. Wu, and P. Phillips, Phys. Rev. Lett. 65, 88 (1990). 3. P. Phillips and H.-L. Wu, Science 252, 1805 (1991). 4. A. Bovier, J. Phys. A 25, 1021 (1992). 5. H.-L. Wu, W. Goff, and P. Phillips, Phys. Rev. B45, 1623 (1992). 6. P. K. Datta, D. Giri, and K. Kundu, Phys. Rev. B 47, 10727 (1993). 7. J. C. Flores and M. Hilke, J. Phys. A 26, L1255 (1993). 8. A. Sánchez and F. Dominguez-Adame, J. Phys. A 27, 3725 (1994). 9. A. Sánchez, E. Maciá, and F. Domínguez-Adame, Phys. Rev. B 49, 147 (1994); 49, 15 428(E) (1994). 10. A. Chakrabarti, S. N. Karmakar, and R. K. Moitra, Phys. Rev. B 50, 13 276 (1994). 11. E. Diez, A. Sánchez, and F. Domínguez-Adame, Phys. Rev. B 50, 14 359 (1994). F. Dominguez-Adame, A. Sanchez, and E. Diez, ibid 50, 17 73.6 (1994). 12. In addition, this calculation pinpoints another difference between RDM and CRDM. In the RDM, the energy is E=q, q being the corresponding wave vector, where in the CRDM its role is played by 2cosq, thus giving rise to more than one band. 13. F. Izrailev, T. Kottos, and G. P. Tsironis (unpublished). 14. N. L. Abbott, J. P. Folkers, G. M. Whitesides, Science 257, 1380 (1992); R. C. Tiberio, H. G. Craighead, M. Lercel, and T. Lau, Appl. Phys. Lett. 62, 476 (1993);G. P. Herman, E. N. Bulgakov, and A. F. Sadreev (unpublished). | |
dspace.entity.type | Publication | |
relation.isAuthorOfPublication | dbc02e39-958d-4885-acfb-131220e221ba | |
relation.isAuthorOfPublication.latestForDiscovery | dbc02e39-958d-4885-acfb-131220e221ba |
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