Abstract
The magnetic equation of state of spin-polarized atomic hydrogen is reported, relating density to magnetic field ($B\ensuremath{\lesssim}10.5$ T), temperature ($T\ensuremath{\gtrsim}300$ mK), and atomic flux used to fill the sample cell. Densities greater than ${10}^{16}$ atoms/${\mathrm{cm}}^{3}$, more than two orders of magnitude greater than initial observations, have been achieved. Results are also presented on the buildup and decay of the density as a function of external conditions. Preliminary observations on the Fermi fluid, atomic deuterium, are reported.
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