Evidence for Two Different Solid Phases of Two Dimensional Electrons in High Magnetic Fields
| dc.creator | Chen, Yong P. | |
| dc.creator | Lewis, R. M. | |
| dc.creator | Engel, L. W. | |
| dc.creator | Tsui, D. C. | |
| dc.creator | Ye, P. D. | |
| dc.creator | Wang, Z. H. | |
| dc.creator | Pfeiffer, L. N. | |
| dc.creator | West, K. W. | |
| dc.date | 2004-07-19 | |
| dc.date.accessioned | 2026-07-07T06:30:16Z | |
| dc.date.available | 2026-07-07T06:30:16Z | |
| dc.description | We have performed RF spectroscopy on very high quality two dimensional electron systems in the high magnetic field insulating phase, usually associated with a Wigner solid (WS) pinned by disorder. We have found two different resonances in the frequency dependent real diagonal conductivity spectrum and we interpret them as coming from \textit{two} different pinned solid phases (labeled as "WS-A" and "WS-B"). The resonance of WS-A is observable for Landau level filling $ν$$<$2/9 (but absent around the $ν$=1/5 fractional quantum Hall effect (FQHE)); it then \textit{crosses over} for $ν$$<$0.18 to the different WS-B resonance which dominates the spectrum at $ν$$<$0.125. Moreover, WS-A resonance is found to show dispersion with respect to the size of transmission line, indicating that WS-A has a large correlation length (exceeding $\sim$100 $μ$m); in contrast no such behavior is found for WS-B. We suggest that quantum correlations such as those responsible for FQHE may play an important role in giving rise to such different solids. | |
| dc.description | 4 pages, 3 figures | |
| dc.identifier | https://arxiv.org/abs/cond-mat/0407472 | |
| dc.identifier | http://arxiv.org/abs/cond-mat/0407472 | |
| dc.identifier | Physical Review Letters 93, 206805 (2004) (slight revised version) | |
| dc.identifier | doi:10.1103/PhysRevLett.93.206805 | |
| dc.identifier.uri | http://salesiana.dossiersoluciones.com/handle/123456789/98299 | |
| dc.subject | Strongly Correlated Electrons | |
| dc.subject | Mesoscale and Nanoscale Physics | |
| dc.title | Evidence for Two Different Solid Phases of Two Dimensional Electrons in High Magnetic Fields | |
| dc.type | text |