Abstract
To the Hubbard model on a square lattice we add an interaction that depends upon the square of a near-neighbor hopping. We use zero-temperature quantum Monte Carlo simulations on lattice sizes up to to show that at half-filling and constant value of the Hubbard repulsion, the interaction triggers a quantum transition between an antiferromagnetic Mott insulator and a superconductor. With a combination of finite-temperature quantum Monte Carlo simulations and the maximum entropy method, we study spin and charge degrees of freedom in the superconducting state. We give numerical evidence for the occurrence of a finite-temperature Kosterlitz-Thouless transition to the superconducting state. Above and below the Kosterlitz-Thouless transition temperature, we compute the one-electron density of states the spin relaxation rate as well as the imaginary and real part of the spin susceptibility The spin dynamics are characterized by the vanishing of and divergence of in the low-temperature limit. As is approached develops a pseudogap feature and below shows a peak at finite frequency.
- Received 10 June 1997
DOI:https://doi.org/10.1103/PhysRevB.56.15001
©1997 American Physical Society