Composite Fermion Hall Conductance at $ν=1/2$
| dc.creator | Lee, D-H | |
| dc.creator | Krotov, Y. | |
| dc.creator | Gan, J. | |
| dc.creator | Kivelson, S. A. | |
| dc.date | 1996-07-22 | |
| dc.date.accessioned | 2026-07-07T03:08:46Z | |
| dc.date.available | 2026-07-07T03:08:46Z | |
| dc.description | We show that in the limit of vanishing bare electron effective mass, and in the presence of particle-hole symmetric disorder (which can be of vanishing strength), the composite fermion Hall conductance is constrained to be $-{1\over 2}\frac{e^2}{h}$. We discuss the implications of this results for the existence and nature of a composite Fermi liquid in the lowest Landau level. | |
| dc.description | 9 pages, RevTeX, 4 PS figures | |
| dc.identifier | https://arxiv.org/abs/cond-mat/9607153 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/9607153 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/27622 | |
| dc.subject | Condensed Matter | |
| dc.title | Composite Fermion Hall Conductance at $ν=1/2$ | |
| dc.type | text |