Evidence for Two Different Solid Phases of Two Dimensional Electrons in High Magnetic Fields
arXiv:cond-mat/0407472 · doi:10.1103/PhysRevLett.93.206805
Abstract
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 2/9 (but absent around the =1/5 fractional quantum Hall effect (FQHE)); it then \textit{crosses over} for 0.18 to the different WS-B resonance which dominates the spectrum at 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 100 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.
4 pages, 3 figures
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