Abstract
A time-differential plunger technique has been used to observe the temporal attenuation of a $gamma$-ray angular distribution. Nuclei of $sup 152$Sm were Coulomb excited by 3 and 4 MeV $alpha$ particles. A dominant static hyperfine interaction was observed from which a magnetic field at the nucleus of 2.6 less than or equal to H (0) less than or equal to 2.9 MOe was deduced. This value is in agreement with the field calculated in the LS scheme. The static interaction may originate in a number of one- and two-electron processes that occur at the target surface. (AIP)
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