The real and imaginary conductivities were plotted in Ω1m1 while they should have been Ω1cm1. The Drude fit from which we extracted the plasma frequency and momentum relaxation rate was incorrectly modeled after the real conductivity which, as we discovered, can be flawed due to irregularities in the phase of the THz transient. We corrected this by modeling the imaginary part of the conductivity [Fig. 1] which has little dependence on the real index of refraction. The key parameters determined from the THz data using the Drude model are not significantly different from those previously reported: the plasma frequency ωp=6.1±0.5THz, the average momentum relaxation time τ=51±6fs, and the mobility μ=89.7cm2Vs for electrons. No other conclusions of the paper are affected.

FIG. 1.

Complex conductivity for the real part σr(v) and the imaginary part σi(v) in the THz region. The dashed line is fitted by the equation σI=ε0ωωp2ω2+τ2 using the parameters τ=51±6fs and ωp=6.1±0.5THz.

FIG. 1.

Complex conductivity for the real part σr(v) and the imaginary part σi(v) in the THz region. The dashed line is fitted by the equation σI=ε0ωωp2ω2+τ2 using the parameters τ=51±6fs and ωp=6.1±0.5THz.

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The authors would like to thank David Cooke and Dr. Hakan Altan for their input.