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The Ghurzi effect indeed leads to a regime with decreasing resistance for increasing temperature, where R ~ l_ee/d^2 (due to
Brownian rather than ballistic flow between walls), but l_ee ~ T^-2 for a Fermi liquid, not T^-5. T^5 comes in at higher temperatures due to the onset of electron-phonon
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scattering. This should be corrected in the text and the figure.
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See original Ghurzi (1963) article cited here, for instance.
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