Developing fractional quantum Hall states at = 17 and 211 in the presence of significant Landau level mixing
Abstract
Termination of the fractional quantum Hall states (FQHSs) and the emergence of Wigner crystal phases at very small Landau level filling factors () have been of continued interest for decades. Recently, in ultra-high-quality, dilute GaAs 2D electron systems (2DESs), strong evidence was reported for FQHSs at =1/7, 2/13 and 2/11 which fall in the = p/(6p1) Jain series of FQHSs, interpreted as integer (p = 1, 2) QHSs of 6-flux composite fermions (6CFs). These states are surrounded by strongly-insulating phases which are generally believed to be Wigner crystals. Here, we study an ultra-high-quality 2DES confined to an AlAs quantum well where the 2D electrons have a much larger effective mass (m* 0.45 me) and a smaller dielectric constant (ε10ε0) compared to GaAs 2D electrons (m* 0.067 me and ε13ε0). This combination of m* and ε renders the Landau level mixing parameter , defined as the ratio of the Coulomb and cyclotron energies, 9 times larger in AlAs 2DESs ( m*/ε). Qualitatively similar to the GaAs 2DESs, we observe an insulating behavior reentrant around a strong =1/5 FQHS, and extending to <1/5. Additionally, we observe a clear minimum in magnetoresistance at =2/11, and an inflection point at =1/7 which is very reminiscent of the first report of an emerging FQHS at =1/7 in GaAs 2DESs. The data provide evidence for developing QHSs of 6CFs at very small fillings. This is very surprising because near 1/6 in our sample is very large (4), and larger has the tendency to favor Wigner crystal states over FQHSs at small fillings. Our data should inspire calculations that accurately incorporate in competing many-body phases of 6CFs at extremely small fillings near =1/6.
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