Non-zero temperature transport near quantum critical points
arXiv:cond-mat/9705206 · doi:10.1103/PhysRevB.56.8714
Abstract
We describe the nature of charge transport at non-zero temperatures () above the two-dimensional () superfluid-insulator quantum critical point. We argue that the transport is characterized by inelastic collisions among thermally excited carriers at a rate of order . This implies that the transport at frequencies is in the hydrodynamic, collision-dominated (or `incoherent') regime, while is the collisionless (or `phase-coherent') regime. The conductivity is argued to be times a non-trivial universal scaling function of , and not independent of , as has been previously claimed, or implicitly assumed. The experimentally measured d.c. conductivity is the hydrodynamic limit of this function, and is a universal number times , even though the transport is incoherent. Previous work determined the conductivity by incorrectly assuming it was also equal to the collisionless limit of the scaling function, which actually describes phase-coherent transport with a conductivity given by a different universal number times . We provide the first computation of the universal d.c. conductivity in a disorder-free boson model, along with explicit crossover functions, using a quantum Boltzmann equation and an expansion in . The case of spin transport near quantum critical points in antiferromagnets is also discussed. Similar ideas should apply to the transitions in quantum Hall systems and to metal-insulator transitions. We suggest experimental tests of our picture and speculate on a new route to self-duality at two-dimensional quantum critical points.
Feedback incorporated into numerous clarifying remarks; additional appendix discusses relationship to transport in dissipative quantum mechanics and quantum Hall edge state tunnelling problems, stimulated by discussions with E. Fradkin
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