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Extended regime of nematic order in an interacting monomer-dimer model of Heilmann and Lieb
We revisit a two-dimensional model of liquid crystals introduced by Heilmann--Lieb (1979), which consists of dimers on the square lattice at chemical potential $λ$, interacting via a hard-core repulsion and an attractive interaction of strength $a>0$ between adjacent, colinear dimers. The model is c
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