Abstract
A two-channel scenario for the conductivity of underdoped is proposed. One is the single-particle excitations channel, which dominates in the optimally doped material, whose resistivity is linear as a function of temperature. The other one gives a contribution which merges the 3D Aslamazov-Larkin fluctuation conductivity at low temperature and obeys a power law at high temperature, depending on two superconductive parameters ( and the zero temperature coherence length ) and an energy scale . This allows one to address the nature of the pseudogap in favor of incoherent pairing.
- Received 21 December 2000
DOI:https://doi.org/10.1103/PhysRevLett.87.197007
©2001 American Physical Society