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By strictly adhering to the microscopic theory of composite fermions (CFs) for the Landau-level filling fractions \nu_e = p/(2 p + 1), we reproduce, with remarkable accuracy, the surface-acoustic-wave (SAW)-based experimental results by Willett and co-workers concerning two-dimensional electron systems with \nu_e close to 1/2. Our results imply that the electron band mass m_b, as distinct from the CF mass m_*, must undergo a substantial increase under the conditions corresponding to \nu_e close to 1/2. We further establish that a finite mean-free path \ell_0 is essential for the observed linearity of the longitudinal conductivity \sigma_{xx}(q) as deduced from the SAW velocity shifts.

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