2015
DOI: 10.1007/s11005-015-0806-6
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Microscopic Conductivity of Lattice Fermions at Equilibrium. Part II: Interacting Particles

Abstract: We apply Lieb-Robinson bounds for multi-commutators we recently derived [BP3] to study the (possibly non-linear) response of interacting fermions at thermal equilibrium to perturbations of the external electromagnetic field. This analysis leads to an extension of the results for quasi-free fermions of [BPH1, BPH2] to fermion systems on the lattice with shortrange interactions. More precisely, we investigate entropy production and charge transport properties of non-autonomous C * -dynamical systems associated w… Show more

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Cited by 9 publications
(73 citation statements)
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“…(iii) Linear response current density: Fix a direction w ∈ R d with w R d = 1 and a (time-dependent) continuous, compactly supported, electric field E ∈ C 0 0 (R; R d ), i.e., the external electric field is a continuous function t → E(t) ∈ R d of time t ∈ R with compact support. Then, as it is explained in Appendix C, [7,21] 1 shows that the space-averaged linear response current observable in the lattice region Λ and at time t = 0 in the direction w is equal to…”
Section: Current Densitiesmentioning
confidence: 92%
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“…(iii) Linear response current density: Fix a direction w ∈ R d with w R d = 1 and a (time-dependent) continuous, compactly supported, electric field E ∈ C 0 0 (R; R d ), i.e., the external electric field is a continuous function t → E(t) ∈ R d of time t ∈ R with compact support. Then, as it is explained in Appendix C, [7,21] 1 shows that the space-averaged linear response current observable in the lattice region Λ and at time t = 0 in the direction w is equal to…”
Section: Current Densitiesmentioning
confidence: 92%
“…In fact, the first term in the right-hand side of (19) corresponds to the paramagnetic coefficient, whereas the second one is the diamagnetic component. For more details, see [21,Theorem 3.7].…”
Section: Current Densitiesmentioning
confidence: 99%
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“…However, it is believed in theoretical physics that electric resistance of conductors should also result from the interactions between charge carriers, and not only from the presence of inhomogeneities (impurities). In [35,36,37], we succeed to extend our previous results to fermion systems with interactions.…”
Section: ]mentioning
confidence: 62%
“…However, there is a plethora [39,40] of other types of elementary excitations not covered by the Bogoliubov theory. We show [32,33,36] that the notion of conductivity measure we defined is nothing else than a spectral measure of the generator of dynamics in an appropriate representation.…”
Section: ]mentioning
confidence: 99%