Brownian motion of a spin in the presence of a magnetic-field gradient can significantly influence the spin-lattice relaxation time. A theory is developed to describe this effect, and experiments on gaseous He³ which confirm the theory in detail are reported. Practical situations where this mechanism can dominate, such as in the construction and use of polarized He³ targets in nuclear-scattering experiments, are discussed. In a homogeneous magnetic field, relaxation times of approximately 7 h at low pressures permit us to establish an upper limit of 7×10^-15e cm for the electric-dipole moment of the He³ nucleus.
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Schearer et al. (1965) studied this question.
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