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Can a gas of spin-up and spin-down fermions become ferromagnetic due to repulsive interactions? This question which has not yet found a definitive theoretical answer was addressed in an experiment with an ultracold two-component Fermi gas.
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The interpretation of the loss rate is complicated since f ( a , T ) f(a,T) is unkown for k F a ≥ 1 k_{F}a\geq 1 . The three body rate f ( a , T ) f(a,T) is expected to be unitarity saturated for k F a ≫ 1 k_{F}a\gg 1 [ 33 ] . The lines in Fig. 2 indicate that the observed loss rate is consistent with unitarity saturation and a sudden drop at the phase transition, which occurs at large values of k F a k_{F}a at higher temperature
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