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facets/D=z/(z-2d) >1, which explains the suppresion of P(f) for small forces with respect to a pure exponential.
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48
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note
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-f.
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50
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note
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Note that in Ref. [25] a somewhat different pressure constraint is employed, since variations in the coordination number may lead to variations in (f) at a fixed pressure.
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note
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We sidestep here the subtle issue of the coarse graining necessary to derive a macroscopic stress field from a microscopic particle model. For a detailed discussion on this, see, e.g., Ref. [48].
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