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x alloys increases linearly, 1.0 microhm cm/atomic % Bi for x < ∼0.2. Assuming the phonon contribution does not change, the resistivity due to impurity scattering is 11 microhm cm for the 11% alloy, etc.
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x alloys increases linearly, 1.0 microhm cm/atomic % Bi for x < ∼0.2. Assuming the phonon contribution does not change, the resistivity due to impurity scattering is 11 microhm cm for the 11% alloy, etc.
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27
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34250874104
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c*.
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c*.
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34250812155
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This work was funded by NSF under contracts DMR-0244570 (M.M.O. and H.H.W, and DMR-0606485 (Z.Z, by the Division of Materials Sciences and Engineering (H.H.W, J.R.T, and Z.Z, Office of Basic Energy Sciences, U.S. Department of Energy under contract DE-AC0500OR22725 with Oak Ridge National Laboratory, managed by UT-Battelle, Limited Liability Corporation; and by National Science Foundation of China Y.J, grant no. 10574113
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This work was funded by NSF under contracts DMR-0244570 (M.M.O. and H.H.W.) and DMR-0606485 (Z.Z.); by the Division of Materials Sciences and Engineering (H.H.W., J.R.T., and Z.Z.), Office of Basic Energy Sciences, U.S. Department of Energy under contract DE-AC0500OR22725 with Oak Ridge National Laboratory, managed by UT-Battelle, Limited Liability Corporation; and by National Science Foundation of China (Y.J.; grant no. 10574113).
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