Abstract

We have measured the effective mass (mm^*) of the four flux composite fermion at Landau level filling factor ν=1/4\nu = 1/4 (4^4CF), using the activation energy gaps at the fractional quantum Hall effect (FQHE) states ν\nu = 2/7, 3/11, and 4/15 and the temperature dependence of the Shubnikov-de Haas (SdH) oscillations around ν=1/4\nu = 1/4. We find that the energy gaps show a linear dependence on the effective magnetic field BeffB_{eff} (BBν=1/4\equiv B-B_{\nu=1/4}), and from this linear dependence we obtain m=1.0mem^* = 1.0 m_e and a disorder broadening Γ\Gamma \sim 1 K for a sample of density n=0.87×1011n = 0.87 \times 10^{11} /cm2^2. The mm^* deduced from the temperature dependence of the SdH effect shows large differences for ν>1/4\nu > 1/4 and ν<1/4\nu < 1/4. For ν>1/4\nu > 1/4, m1.0mem^* \sim 1.0 m_e. It scales as Bν\sqrt{B_{\nu}} with the mass derived from the data around ν=1/2\nu =1/2 and shows an increase in mm^* as ν1/4\nu \to 1/4, resembling the findings around ν=1/2\nu =1/2. For ν<1/4\nu < 1/4, mm^* increases rapidly with increasing BeffB_{eff} and can be described by m/me=3.3+5.7×Beffm^*/m_e = -3.3 + 5.7 \times B_{eff}. This anomalous dependence on BeffB_{eff} is precursory to the formation of the insulating phase at still lower filling.Comment: 5 pages, 3 figure

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