Abstract
Nuclear spin-lattice relaxation rates 1/T1 in weakly antiferromagnetic metals are studied by using the renormalized spin fluctuation theory. Above the Néel temperature TN the theory predicts that 1/T1 is proportional to T⁄(T−TN)1⁄2. Below TN the importance of anisotropy and magnetostriction is pointed out and the result predicts that 1/T1 is proportional to T⁄M(T), where M(T) is the staggered magnetization. Some numerical examples based on the electron gas model with Umklapp processes are shown.