Magnetic scaling in cuprate superconductors

We determine the magnetic phase diagram for the YBa₂{Cu}₃O₆₊ₓ and La_2-x{Sr}ₓCuO₄ systems from various NMR experiments. We discuss the possible interpretation of NMR and neutron scattering experiments in these systems in terms of both the nonlinear {σ} model of nearly localized spins and a nearly antiferromagnetic Fermi liquid description of magnetically coupled quasiparticles. We show for both the 2:1:4 and 1:2:3 systems that bulk properties, such as the spin susceptibiltiy, and probes at the antiferromagnetic wave vector ({π},{π}), such as ⁶³{T}₁$, the $⁶³Cu$ spin-lattice relaxation time, both display a crossover at a temperature ${T}cr$, which increases linearly with decreasing hole concentration, from a nonuniversal regime to a z=1 scaling regime characterized by spin pseudogap behavior. We pursue the consequences of the ansatz that Tcr corresponds to a fixed value of the antiferromagnetic correlation length {ξ} and show how this enables one to extract the magnitude and temperature dependence of {ξ} from measurements of T₁ alone. We show that like Tcr, the temperature T* which marks a crossover at low temperatures from the z=1 scaling regime to a quantum disordered regime, exhibits the same dependence on doping for the 2:1:4 and 1:2:3 systems, and so arrive at a unified description of magnetic behavior in the cuprates, in which the determining factor is the planar hole concentration.