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note
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F.
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56
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15444376969
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note
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imp]=[O(r,σ),H], where O is any operator that does not explicitly depend on p. Both the particle and spin density are such operator and thus the equations of motion remain the same in the presence of impurities. The complications due to the impurities appear in the calculation of the average values of the operators.
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57
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15444364641
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note
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0s and α=0. Thus, the dc spin conductivity vanishes for any dissipation mechanism. The same follows directly from the other magnetization components and in the case of α≠0.
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