We show that the differential contribution, at energy E, to the persistent currents of independent electrons in infinitely extended quantum systems is given by (2{π}i)^-1{{{∂}}}_{{{φ}}}$ [ln detS(E,{φ})]dE, where S(E,{φ}) is the (on-shell) scatteirng matrix. We apply this result to the calculation of the persistent currents in two examples: a mesoscopic loop connected to one infinitely long lead, and a plane pierced by a flux line. In the last example spin plays a remarkable role.
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Akkermans et al. (1991) studied this question.
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