Abstract
Translational invariance properties of the single‐particle distribution function D1(x, L, z) of the grand canonical ensemble are investigated for a one‐dimensional hard‐core fluid. For a fluid of finite length L it is shown that D1(x, L, z) is nowhere constant. It is shown that, in the thermodynamic limit and for x far from either wall, D1(x, L, z) is a constant equal to the grand canonical density ρ.

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