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the direct numerical simulations [24, 25]. In particular in [26] the principle possibility to derive the nonclassical exponents for molecular liquids basing on the specific closure of the Ornstein-Zernike equation. 

The proposed global isomorphism between LJ fluids and LG leads to the conclusion that the phase coexistence region of the latter is nothing but isomorphic image of the corre- sponding region of the phase diagram of the LG. For example applying the isomorphism transformation (8) to the known result for 2D Ising model [27]: 

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