J. Phys. Soc. Jpn. 81 (2012) 023701 (4 pages) |Previous Article| |Next Article| |Table of Contents|
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(Received July 12, 2011; Revised October 11, 2011; Accepted November 22, 2011; Published January 5, 2012)
The question of conductivity is revisited. Using the total momentum shift operator to construct the perturbed many-body Hamiltonian and ground state wave function the second derivative of the ground state energy with respect to the perturbing field is expressed in terms of the one and two-body momentum densities. The distinction between the adiabatic and envelope function derivatives, hence that between the Drude and superfluid weights, can be introduced in a straightforward manner. It is shown that a discontinuity in the momentum density leads to a contribution to the Drude weight, but not the superfluid weight, however a δ-function contribution in the two-body momentum density (such as in the BCS wave-funtion) contributes to both quantities. The connection between the discontinuity in the momentum density and localization is also demonstrated. ©2012 The Physical Society of Japan
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http://jpsj.ipap.jp/link?JPSJ/81/023701/
DOI: 10.1143/JPSJ.81.023701