Abstract
Theory of magnetic-induction bifurcation in the Condon domain phase of a three-dimensional (3D) electron gas under high-magnetic field is presented. The results\char22{}the diamagnetic phase transition temperature and the induction bifurcation values\char22{}are in good agreement with nuclear magnetic resonance data in silver. The temperature dependence of the order parameter of the diamagnetic phase transition\char22{}the magnetization in each Condon domain\char22{}is obtained by a comparison of the theory with the experiment. The mean-field approach has been shown to lead to the universal behavior of an electron gas of 2D and 3D dimensionality.
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