Abstract
Gap anisotropy strongly affects the temperature dependence of nuclear-spin–lattice relaxation in the superconducting state. A model is presented which contains a simple form for the gap anisotropy expected of a weakly coupled system of superconducting layers. Phonon-induced quasiparticle damping is also included and is shown to contribute significantly to the relaxation rate. This is in contrast to the case of conventional superconductivity where phonons play only a minor role. The presence of both gap anisotropy and phonon quasiparticle damping eliminate the usual BCS T11 enhancement below Tc, in agreement with experiments on YBa2 Cu3 O7.