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The percolation properties of two-dimensional rotationally invariant granular random elastic networks (the disk model) are studied by use of both numerical simulations and finite-size scaling analysis. For the case of normal--empty-bond random networks, an exponent f{}3.2±{}0.4, which governs the behavior of the network elasticity above percolation threshold pc, is found to be the same as the corresponding exponent for the bond-bending force model studied earlier. For the case of rigid--normal-bond networks, a new exponent c{}1.02±{}0.07 which governs the elasticity below pc is found, which is close to but smaller than the superconductivity exponent s. These results can be understood qualitatively by use of the nodes-links-blobs picture of percolation backbones and scaling arguments.
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Shechao Feng (1985) studied this question.
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