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On the example of two-dimensional (2D) 3He we demonstrate that the main universal features of its experimental temperature T - density x phase diagram [see M. Neumann, J. Ny'{e}ki, J. Saunders, Science 317, 1356 (2007)] look like those in the heavy-fermion metals. Our comprehensive theoretical analysis of experimental situation in 2D 3He allows us to propose a simple expression for effective mass M^(T,x), describing all diverse experimental facts in 2D 3He in unified manner and demonstrating that the universal behavior of M^(T,x) coincides with that observed in HF metals.

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