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3 term has been used to describe dephasing above 1 K in similar samples in Refs. 3 and 9, among others.
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During the course of the Ag experiment, we slightly underestimated the effect of heating due to the drive current. Since electron cooling at the lowest temperatures occurs almost entirely by thermal conduction through the leads, one can calculate the effect of heating using the Weidemann-Franz relation and the known sample geometry. The drive current at the lowest three temperatures shown was 5 nA, which at 50 mK causes a temperature rise of about 5 mK at the center of the wire. Use of a lower drive current might result in a slightly larger value of p from the fit. This error was corrected in the Cu experiment, where electron heating due to the drive current was kept below a few percent of the lattice temperature.
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