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We discuss the spin fluctuations and the role played by the magnetic susceptibility in an atomic Fermi gas interacting with positive scattering length.
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G. J. Conduit and E. Altman, http://arxiv.org/abs/0911.2839
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S.-Y. Chang, M. Randeria, N. Trivedi, http://arxiv.org/abs/1004.2680
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In particular for a clean and not polarised system the transition is “weakly” first order till a certain temperature, above which is second order. In the most recent Monte-Carlo calculation giorgini at T = 0 T=0 for cold gases is very hard to distinguish whether the transition is of first or of the second order and a divergent behaviour of χ \chi is clearly found (see giorgini and Fig. 1
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