Local Moments Coupled to a Strongly Correlated Electron Chain
arXiv:cond-mat/9511069 · doi:10.1103/PhysRevB.53.R488
Abstract
A 1D model hamiltonian that is motivated by the recent discovery of the heavy-fermion behavior in the cuprates of the type is studied. It consists of interacting conduction electrons coupled to a lattice of localized spins through a Kondo exchange term . Exact diagonalization and density matrix renormalization group methods are used. The latter method is generalized to arbitrary densities. At half-filling, a spin gap opens for all . Away from half-filling it is shown that, at strong % , the ground state is an unsaturated ferromagnet . At weak the system is in a paramagnetic phase with enhanced RKKY correlations. The importance of self-screening of the local moments in the depletion regime is discussed. We argue that these findings transcend the specifics of the model.
10 pages, Latex, 4 figures included, to be published in PRB (Rapid Communications)