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When heating the sample, the conductance peak at Δ/e in the dI/dV(V) characteristic taken at U = 0 split into two peaks, as expected from the presence of a minigap in the density of states in the wire [see W. Belzig, C. Bruder, and A. L. Fauchere, Phys. Rev. B 58, 14 531 (1998); F K. Wilhelm and A. A. Golubov, Phys. Rev. B 62, 5353 (2000)].
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When heating the sample, the conductance peak at Δ/e in the dI/dV(V) characteristic taken at U = 0 split into two peaks, as expected from the presence of a minigap in the density of states in the wire [see W. Belzig, C. Bruder, and A. L. Fauchere, Phys. Rev. B 58, 14 531 (1998); F K. Wilhelm and A. A. Golubov, Phys. Rev. B 62, 5353 (2000)].
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The collision term corresponding to phonon emission is important for data taken on long wires at large voltages. The addition of this term to the electron-electron collision term in the Boltzmann equation suffices to account for the measured distribution functions in silver wires, without any ad hoc assumption [13].
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3 dependence of the energy transfer rate between electrons and phonons reported, for example, in M. L. Roukes, M. R. Freeman, R. S. Germain, R. C. Richardson, and M. B. Ketchen, Phys. Rev. Lett. 55, 422 (1985).
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