Abstract
Based on the formal similarity between perturbations governing gyromagnetic ratio shifting and spin relaxation of alkali atoms in collisions with rare-gas atoms, a relatively direct semiempirical estimate of the gj shift as a function of buffer-gas density can be achieved. The expression ΔgJgJ=(43π)12nσdis12σkin is obtained for the fractional shift in gJ, where n is the rare-gas number density, σkin the alkali-rare-gas kinetic cross section, and σdis the cross section for alkali spin disorientation. With this relationship, we predict a fractional gJ shift for Rb by He equal to -5. 3 × 1011 Torr1, as compared with a recent value, -(5±3) × 1011 Torr1, obtained through measurement by Hayne, Robinson, and their co-workers.

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