We have studied the nuclear magnetic resonance of Al²⁷ nuclei in very dilute alloys of Mn ({≤}0.049 at.%), Fe({≤}0.045 at.%), and Cu({≤}0.30 at.%) in Al. The room-temperature results show line intensities that decrease rapidly with increasing impurity concentration. This decrease is attributed to a wipe-out from the resonance of the Al²⁷ nuclei in the vicinity of the impurity, as a result of the interaction of the Al²⁷ quadrupole moment with the local oscillating electric-field gradients. The experimental results indicate a wipe-out for the Al:Mn and Al:Fe alloys that is considerably larger than that for the corresponding Al:Cu alloys. This large electrostatic interaction in the case of the transition-metal impurities with unfilled d shells is in agreement with the Friedel-Anderson model for such alloys, which describes the screening in terms of resonant scattering of the host-metal conduction electrons by virtual d states localized at the impurity site. Using this model, one predicts an increase in the oscillating field gradient on going from Al:Cu to Al:Mn in agreement with experiment. Linewidth measurements in the liquid-helium temperature range show no temperature or magnetic-field dependence, indicating there is no local moment on the impurities.
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Brettell et al. (1967) studied this question.
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