We study rigidity transitions in covalent amorphous networks using size-increasing cluster approximations and constraint-counting algorithms. Possible consequences of the presence of self-organization are examined. The analysis reveals two transitions instead of the usual (mean-field) single transition: one from a floppy to an isostatic rigid phase at a mean coordination number c1 where the number of floppy modes vanishes and a second one from an isostatic to a stressed rigid phase at c2 . The value of the two critical mean coordination numbers as well as the width Δ = c2 − c 1 of the intermediate phase depend very strongly on the presence of medium-range order elements such as rings.
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